EUROPEAN JOURNAL OF PURE AND APPLIED MATHEMATICS 2025, Vol. 18, Issue 1, Article Number 5725 ISSN 1307-5543 – ejpam.com Published by New York Business Global New Study of Prabhakar Operators Associated With Inequalities and Its Significant Applications With Different Convexity Rana Safdar Ali1,∗, Nazia Yaseen1, Gauhar Rahman2, Ahmad Aloqaily3, Nabil Mlaiki3 1 Department of Mathematics and Statistics, Faculty of Science, The University of Lahore, Sargodha Campus, Sargodha, Punjab, Pakistan 2 Department of Mathematics and Statistics, Faculty of Science, Hazara University, Mansehra, KPK, Pakistan 3 Department of Mathematics and Sciences, Prince Sultan University, Riyadh 11586, Saudi Arabia Abstract. Convexity plays a dominant role in the modification of fractional inequalities. Most fractional inequalities are proved based on different types of convexity and fractional operators, which have immense applications in various areas of mathematics. This article aims to investigate the Hermite-Hadamard type inequalities with a different kind of convexity by the implementation of Prabhakar fractional operators. Moreover, we discuss the behavior of trapezoidal type inequalities for the h-Godunova-Levin pre-invex function through Prabhakar fractional operators. Additionally, we present a comparison of our findings with existing literature, which are summarized through corollaries. 2020 Mathematics Subject Classifications: 26A51, 26D10,2 6A33, 26D20 Key Words and Phrases: Convexity, Hermite-Hadamard inequalities, Prabhaker fractional integral operators, trapezoid inequalities 1. Introduction Fractional integrals and inequalities define an essential area of research in the field of mathematical analysis and its great applications [1, 16–19, 21–23]. These notions are a generalization of classical integral inequalities and provide important new ideas with wide areas of eventual application. With regard to the integral type of inequalities, it is also observed that an impressive development has been achieved in this area of study as these inequalities are becoming more significant to pure and applied mathematics [6, 14]. ∗Corresponding author. DOI: https://doi.org/10.29020/nybg.ejpam.v18i1.5725 Email addresses: rsafdar0@gmail.com (R. S. Ali), naziaimran145@gmail.com (N. Yaseen), gauhar55uom@gmail.com (G. Rehman), maloqaily@psu.edu.sa (A. Aloqaily), nmlaiki@psu.edu.sa; nmlaiki2012@gmail.com (N. Mlaiki) https://www.ejpam.com 1 Copyright: © 2025 The Author(s). (CC BY-NC 4.0) R. S. Ali et al. / Eur. J. Pure Appl. Math, 18 (1) (2025), 5725 2 of 14 The development of the theory of convexity, which is very closely linked to inequality, has progressed considerably. It is worth noting that convex functions are very important in the study and derivation of many integral inequalities [3, 7, 8]. One such is the well-known Hermite-Hadamard inequality. Formulated by Charles Hermite in 1881 and modernized by Jacques Hadamard in 1893, the inequality has been a part of fundamental concepts of convexity . The historical background of the Hermite-Hadamard inequality would suggest that it thrived long before the mid-1970s revival by Dragoslav Mitrinović, who published several books on the history of mathematics in general and convex inequalities in particular [9, 15]. Recently, various generalizations have turned the studies in inequality areas to another range. The classical structure of differentiable convex functions was broadened by the term invexity, introduced in 1981 by Robert Hanson [13], and so new optimization and analysis areas could be developed . Building on this, Mond [28] and Weir [27] further developed the notion of preinvexity, which has been helpful in perfecting optimization theory . Further advancements have been inclusive of various generalized concepts of convexity that were defined. Dragomir [7] presented the s-Godunova-Levin type convexity, which has been the focus of many studies in the subsequent period [20]. Moreover, the produc- tive concept of h-convexity by Varošanec [26] and also h-Godunova-Levin convexity and preinvexity by Almutari [4] opened new avenues and methods in this area . This paper study h-Godunova-Levin types of convex and preinvex functions and the fractional integral operators, including the Mittag-Leffler functions, to achieve the new fractional Hermite-Hadamard and the trapezoid inequalities. 2. Preliminaries In this section, we discuss the basic definitions which help to understand our main results. Definition 1. [2] A function § : I → R is termed convex if it satisfies the following condition: §[tos̊+ (1− to)æ] ≤ to§(̊s) + (1− to)§(æ), for all to ∈ [0, 1], s̊,æ ∈ I. Building upon this concept of convexity, we can establish the Hermite-Hadamard (H-H) type inequality as: § ( s̊+æ 2 ) ≤ 1 æ− s̊ ∫ æ s̊ §(to) dto ≤ §(̊s) + §(æ) 2 . (1) Numerous related results are presented in [25], assuming s̊,æ ∈ I ⊆ Rand̊s < æ. Definition 2. [24] Consider an invex set I ⊆ R defined in relation to a bifunction § : I × I → R. For æ, s̊ ∈ I and λ ∈ [0, 1], we define: s̊+ λ§(æ, s̊) ∈ I R. S. Ali et al. / Eur. J. Pure Appl. Math, 18 (1) (2025), 5725 3 of 14 Definition 3. [24] A function § : I → R is called preinvex for æ, s̊ ∈ I and to ∈ [0, 1] if: §(̊s+ toζ(æ, s̊)) ≤ to§(æ) + (1− to)§(̊s), where I is an invex set relative to the binary function ζ. Definition 4. [10] A function § : I ⊆ R → R, which takes only positive values, is known as a Godunova-Levin function if, for all æ, s̊ ∈ I and to ∈ (0, 1), the following inequality holds: §(toæ+ (1− to)̊s) ≤ §(æ) to + §(̊s) 1− to , for all æ, s̊ ∈ I, to ∈ (0, 1). Definition 5. [4] Assume h : (0, 1) → R is a non-negative function. We say a function § : I → R is h-Godunova-Levin if, for any æ, s̊ ∈ I and to ∈ (0, 1), the following inequality holds: §(toæ+ (1− to)̊s) ≤ §(æ) h(to) + §(̊s) h(1− to) . Definition 6. [4] A function § : I → R is called h-Godunova-Levin preinvex with respect to ζ if, for any æ, s̊ ∈ I and to ∈ (0, 1), the inequality §(æ + toζ (̊s,æ)) ≤ §(æ) h(1− to) + §(̊s) h(to) , is satisfied. Definition 7. [12] Let § ∈ L1[æ, s̊], then the Riemann-Liouville left and right fractional integrals are defined as follows: Iαæ+§(z) = 1 Γ(α) ∫ z æ (z − u)α−1§(u) du, z > æ, Iαs̊−§(z) = 1 Γ(α) ∫ s̊ z (u− z)α−1§(u) du, z < s̊. Definition 8. [29] The gamma function is defined by the following integral representation: Γ(z) = ∫ +∞ 0 uz−1e−udu, for ℜ(z) > 0. Definition 9. [29] The Pochhammer symbol is defined as follows: (z)k = { 1, for k = 0, z ̸= 0, z(z + 1) · · · (z + k − 1), for k ≥ 1. For k ∈ N and z ∈ C. (z)k = Γ(z + k) Γ(z) , where Γ is the gamma function. R. S. Ali et al. / Eur. J. Pure Appl. Math, 18 (1) (2025), 5725 4 of 14 Definition 10. [5] The Mittag-Leffler function of three parameters: Eα β,γ(w; p) = +∞∑ n=0 (γ)n Γ(βn+ α) wn n! , (w,α, β, γ ∈ C,ℜ(β) > 0). Definition 11. [11] Let α, β, γ ∈ C,ℜ(α) > 0,ℜ(β) > 0. Let § ∈ L1[æ, s̊] and x ∈ [æ, s̊]. Then the left-sided and the right-sided Prabhakar fractional operators Jα,γ β;æ+§ and Jα,γ β ;̊s−§, are defined by ( Jα,γ β;æ+§ ) (x; r) = ∫ x æ (x− t)β−1Eα β,γ (ω(x− t)α; r) §(t)dt,( Jα,γ β ;̊s−§ ) (x; r) = ∫ s̊ x (t− x)β−1Eα β,γ (ω(t− x)α; r) §(t)dt. In this work, the following notations will be used:( Jæ + s̊,β ) (ω, §) = ( Jα,γ β;æ+§ ) (̊s, p)( Js̊ − æ,β ) (ω, §) = ( Jα,γ β ;̊s−§ ) (æ; p) 3. Fractional Analysis of the Hermite-Hadamard (H-H) type Inequalities via h-Godunova-Levin convexity (h-GL). This section focuses on deriving Hermite-Hadamard type inequalities for h-Godunova- Levin convex functions by means of the Fractional Function Operator, which is detailed below. Theorem 1. Let § : [æ, s̊] → R be an h-Godunova-Levin convex function, where 0 < æ < s̊ and § ∈ L1[æ, s̊]. Assume h : (0, 1) → R is a positive function with h(to) ̸= 0 ; then, h(1/2) 2 § ( æ+ s̊ 2 )( Js̊ − æ,β ) ( ω′, 1 ) ≤ 1 2 [( ℑs̊− æ,β ) ( ω′, § ) + ( Jæ + s̊,β ) ( ω′, § )] ≤ §(æ) + §(̊s) 2 ∫ 1 0 [ 1 h(to) + 1 h(1− to) ] (1− to) β−1Jαβ,γ (ω(1− to) α; p) dto, ω′ = ω (̊s− æ)α . Proof. Using the h -Godunova-Levin convexity of § on [æ, s̊] , let m,n ∈ [æ, s̊], and we obtain §((η)m+ (1− η)n) ≤ §(m) h(η) + §(n) h(1− η) (2) For putting the values m = toæ + (1 − to)̊s, n = (1 − to)æ + tos̊ and η = 1 2 in equation (2), we have § ( æ+ s̊ 2 ) ≤ 1 h(1/2) [§(toæ+ (1− to)̊s) + §((1− to)æ + tos̊)] (3) R. S. Ali et al. / Eur. J. Pure Appl. Math, 18 (1) (2025), 5725 5 of 14 Multiplying each side by (1−to) β−1Jαβ,γ (ω(1− to) α; p) and integrate the resultant inequal- ity on [0, 1] in terms of to in the equation (3), we have § ( æ+ s̊ 2 )∫ 1 0 (1− to) β−1Jαβ,γ (ω(1− to) α; p) dto ≤ 1 h(12) ×[ ∫ 1 0 (1− to) β−1Jαβ,γ (ω(1− to) α; p) §(toæ+ (1− to)̊s)dto + ∫ 1 0 (1− to) β−1Jαβ,γ (ω(1− to) α; p) §((1− to)æ + tos̊)dto ] § ( æ+ s̊ 2 ) +∞∑ n=0 (γ)n Γ(βn+ α) wn n! ∫ 1 0 (1− to) αn+β−1dto ≤ 1 h(1/2) +∞∑ n=0 (γ)n Γ(βn+ α) wn n! × [∫ 1 0 (1− to) αn+β−1§(toæ+ (1− to)̊s)dto + ∫ 1 0 (1− to) αn+β−1§((1− to)æ + tos̊)dto ] (4) By evaluating the integrals in inequality (4), we obtain h(1/2) 2 § ( æ+ s̊ 2 )( Js̊ − æ,β ( ω′, 1 )) ≤ 1 2 [( Jæ + s̊,β ) ( ω′; § ) + ( Js̊ − æ,β ) ( ω′; § )] (5) For the second half of the inequality, we similarly employ the h-Godunova-Levin con- vexity of §, we have §(toæ+ (1− to)̊s) ≤ §(æ) h(to) + §(̊s) h(1− to) §((1− to)æ + tos̊) ≤ §(æ) h(1− to) + §(̊s) h(to) After adding the above inequalities, we have §(toæ+ (1− to)̊s) + §((1− to)æ + tos̊) ≤ (§(æ) + §(̊s)) [ 1 h(to) + 1 h(1− to) ] (6) Multiplying both sides by (1 − to) β−1Jαβ,γ (ω(1− to) α; p) and integrating the resultant inequality on [0, 1] with respect to to in equation (6), we obtain[∫ 1 0 (1− to) β−1Jαβ,γ (ω(1− to) α; p) §(toæ+ (1− to)̊s)dto ] + [∫ 1 0 (1− to) β−1Jαβ,γ (ω(1− to) α; p) §((1− to)æ + tos̊)dto ] ≤ (§(æ) + §(̊s)) ∫ 1 0 [ 1 h(to) + 1 h(1− to) ] (1− to) β−1Jαβ,γ (ω(1− to) α; p) dto (7) R. S. Ali et al. / Eur. J. Pure Appl. Math, 18 (1) (2025), 5725 6 of 14 After solving the equation (7), we have 1 2 [( Jæ + s̊,β ) (ω′, §) + ( Js̊ − æ,β ) ( ω′; § )] ≤ §(æ) + §(̊s) 2 ∫ 1 0 [ 1 h(to) + 1 h(1− to) ] (1−to) β−1Jαβ,γ (ω(1− to) α; p) dto (8) Combining the equations (5) and (8), we obtain h(1/2) 2 § ( æ+ s̊ 2 )( Js̊ − æ,β ) ( ω′, 1 ) ≤ 1 2 [( ℑs̊− æ,β ) ( ω′, § ) + ( Jæ + s̊,β ) ( ω′, § )] ≤ §(æ) + §(̊s) 2 ∫ 1 0 [ 1 h(to) + 1 h(1− to) ] (1− to) β−1Jαβ,γ (ω(1− to) α; p) dto Corollary 1. Taking h(to) = tso in Theorem (1), we derive an inequality of the (H-H) type for s-Godunova-Levin (GL) type convex functions: (1/2)s 2 § ( æ+ s̊ 2 )( Js̊ − æ,β ) ( ω′, 1 ) ≤ 1 2 [( Js̊ − æ,β ) ( ω′, § ) ≤ §(æ) + §(̊s) 2 ∫ 1 0 [ 1 tso + 1 (1− to)s ] (1− to) β−1Jαβ,γ (ω(1− to) α; p) dto Corollary 2. By selecting h(to) = 1 in Theorem (1), we derive an inequality of the (H-H) type for the p function: 1 2§ ( æ+s̊ 2 ) ( Js̊ − æ,β ) (ω′, 1) ≤ 1 2 [( ℑs̊− æ,β ) (ω′, §) + ( ℑæ+ s̊,β ) (ω′, §) ] ≤ (§(æ) + §(̊s)) ( Jæ + s̊,β ) (ω′, 1) Corollary 3. Selecting h(to) = 1/to in Theorem (1), an inequality of the (H-H) type is derived for functions that are convex: § ( æ+s̊ 2 ) ( Js̊ − æ,β ) (ω′, 1) ≤ 1 2 [( ℑs̊− æ,β ) (ω′, §) + ( ℑæ+ s̊,β ) (ω′, §) ] ≤ §(æ)+§(̊s) 2 ( Jæ + s̊,β ) (ω′, 1) Corollary 4. By choosing h(to) = to in Theorem (1), we obtain an (H-H) type inequality for (G-L) functions: 1 4§ ( æ+s̊ 2 ) ( Js̊ − æ,β ) (ω′, 1) ≤ 1 2 [( Js̊ − æ,β ) (ω′, §) + ( Jæ + s̊,β ) (ω′, §) ] ≤ §(æ)+§(̊s) 2 ∫ 1 0 [ (1−to)β−2 1−to ] Jαβ,γ (ω(1− to) α; p) dto Corollary 5. Choosing h(to) = 1/tso in Theorem (1), we obtain an (H-H) type inequality for s-convex functions: 2s−1§ ( æ+s̊ 2 ) ( ℑs̊− æ,β ) (ω′, 1) ≤ 1 2 [( ℑs̊− æ,β ) (ω′, §) + ( Jæ + s̊,β ) (ω′, §) ] ≤ §(æ)+§(̊s) 2 ∫ 1 0 [tso + (1− to) s] (1− to) β−1Jαβ,γ (ω(1− to) α; p) dto R. S. Ali et al. / Eur. J. Pure Appl. Math, 18 (1) (2025), 5725 7 of 14 4. On Trapezoidal-Type Inequalities for Prabhakar Functions with Preinvexity Properties of the h-Godunova-Levin Type In this section, we prove a lemma concerning Prabhakar fractional operators that possess the h-Godunova-Levin preinvexity property. This lemma is crucial for supporting the derivation of our main results. Lemma 1. Let § : I = [æ,æ+ ζ (̊s,æ)] → R be a differentiable function, and let I be a set that is invex with respect to ζ : I × I → R, where ζ (̊s,æ) > 0 for all s̊,æ ∈ I. Then §(æ) + §(æ + ζ (̊s,æ)) 2 ℑα β,γ(ω; p)− 1 2ζ (̊s,æ)β−1 (9) × [( Jæ + æ+ζ (̊s,æ),β−1 ) ( ω′; § ) + ( J (æ+ζ (̊s,æ))− æ,β−1 ) ( ω′; § )] = ζ (̊s,æ) 2 I where I = ∫ 1 0 (1− to) β−1Jαβ,γ (ω(1− to) α; p) §′(æ + toζ (̊s,æ))dto + ∫ 1 0 (−to) β−1Jαβ,γ (ω(to) α; p) §′(æ + toζ (̊s,æ))dto, and ω′ = (ω/ζ (̊s,æ)α). Proof. Consider the integral I = ∫ 1 0 (1− to) β−1Jαβ,γ (ω(1− to) α; p) §′(æ + toζ (̊s,æ))dto + ∫ 1 0 (−to) β−1Jαβ,γ (ω(to) α; p) §′(æ + toζ (̊s,æ))dto (10) Let I = I1 + I2 First, we take the fractional integral I1, we have I1 = +∞∑ s̊=0 (γ)n Γ(βn+ α) wn n! ∫ 1 0 (1− to) β−1+αn§′(æ + toζ (̊s,æ))dto Taking the integration by parts, we have I1 = +∞∑ n=0 (γ)n Γ(βn+ α) wn n! ×[ (1− to) β+αn−1 §(æ + toζ (̊s,æ)) ζ (̊s,æ) ∣∣∣∣1 0 −β + αn− 1 ζ (̊s,æ) ∫ 1 0 (1− to) β+αn−2§(æ + toζ (̊s,æ))dto ] I1 = +∞∑ n=0 (γ)n Γ(βn+ α) wn n! R. S. Ali et al. / Eur. J. Pure Appl. Math, 18 (1) (2025), 5725 8 of 14 × [ (æ + ζ (̊s,æ)) ζ (̊s,æ) − β + αn− 1 ζ (̊s,æ) ∫ 1 0 (1− to) β+αn−2§(æ + toζ (̊s,æ))dto ] I1 = §(æ + ζ (̊s,æ)) ζ (̊s,æ) ℑα β,γ(ω; p)− 1 (ζ (̊s,æ))β ( Jæ + æ+ζ (̊s,æ),β−1 ) ( ω′, § ) Continuing in the same manner, we obtain I2 = §(æ) ζ (̊s,æ) Jαβ,γ(ω; p)− 1 (ζ (̊s,æ))β ( J æ+ζ (̊s,æ)− æ,β−1 ) ( ω′, § ) I = §(æ) + §(æ + ζ (̊s,æ)) ζ (̊s,æ) Jαβ,γ(ω; p)− 1 (ζ (̊s,æ))β × [( J (æ+ζ (̊s,æ))− æ,β−1 ) ( ω′, § ) + ( Jæ + æ+ζ (̊s,æ),β−1 ) ( ω′, § )] By multiplying by ζ (̊s,æ)/2, we obtain §(æ) + §(æ + ζ (̊s,æ)) 2 ℑα β,γ(ω; p)− 1 2ζ (̊s,æ)β−1 × [( Jæ + æ+ζ (̊s,æ),β−1 ) ( ω′; § ) + ( J (æ+ζ (̊s,æ))− æ,β−1 ) ( ω′; § )] = ζ (̊s,æ) 2 I By Lemma 1, we present the following theorem. Theorem 2. Consider a function §: I=[æ, æ+ ζ (̊s,æ)] −→ (0,+∞)withI ∈ R, and let it be a differentiable function on I. Also, suppose that |§′| is a h-Godunova-Levin preinvex function on I; then, §(æ) + §(æ + ζ (̊s,æ)) 2 Jαβ,γ(ω; p)− 1 2ζ (̊s,æ)β−1 × [( Jæ + æ+ζ (̊s,æ),β−1 ) ( ω′, § ) + ( J (æ+ζ (̊s,æ))− æ,β−1 ) ( ω′, § )] ≤ ζ (̊s,æ) 2 (∣∣§′(æ)∣∣+ ∣∣§′(̊s)∣∣) ∫ 1 0 +∞∑ n=0 ∣∣∣∣ (γ)n Γ(βn+ α) wn n! ∣∣∣∣ × ∣∣∣∣(1− to) β+αn−1 − (to) β+αn−1 h(to) ∣∣∣∣ dto. Proof.∣∣∣∣ §(æ) + §(æ + ζ (̊s,æ)) 2 Jαβ,γ(ω; p)− 1 2ζ (̊s,æ)β−1 × [( ℑæ+ æ+ζ (̊s,æ),β−1 ) ( ω′, § ) + ( ℑ(æ+ζ (̊s,æ))− æ,β−1 ) ( ω′, § )] | R. S. Ali et al. / Eur. J. Pure Appl. Math, 18 (1) (2025), 5725 9 of 14 = ∣∣∣∣ζ (̊s,æ)2 I ∣∣∣∣ ≤ ζ (̊s,æ) 2 +∞∑ n=0 ∣∣∣∣ (γ)n Γ(βn+ α) wn n! ∣∣∣∣ ∫ 1 0 ∣∣∣(1− to) β+αn−1 − (to) β+αn−1 ∣∣∣ ∣∣§′(æ + toζ (̊s,æ)) ∣∣dto ≤ ζ (̊s,æ) 2 +∞∑ n=0 ∣∣∣∣ (γ)n Γ(βn+ α) wn n! ∣∣∣∣ × ∫ 1 0 ∣∣∣(1− to) β+αn−1 − (to) β+αn−1 ∣∣∣ ∣∣∣∣§′(æ)h(to) + §′(̊s) h(1− to) ∣∣∣∣ dto ≤ ζ (̊s,æ) 2 +∞∑ n=0 ∣∣∣∣ (γ)n Γ(βn+ α) wn n! ∣∣∣∣ × [∣∣§′(æ)∣∣ ∫ 1 0 ∣∣∣(1− to) β+αn−1 − (to) β+αn−1 ∣∣∣ 1 h(to) dto + |§′(̊s) ∣∣∣∣∫ 1 0 ∣∣∣(1− to) β+αn−1 − (to) β+αn−1 ∣∣∣ 1 h(1− to) dto = ζ (̊s,æ) 2 (∣∣§′(æ)∣∣+ ∣∣§′(̊s)∣∣) ∫ 1 0 +∞∑ n=0 ∣∣∣∣ (γ)n Γ(βn+ α) wn n! ∣∣∣∣ × ∣∣∣∣(1− to) β+αn−1 − (to) β+αn−1 h(to) ∣∣∣∣dto. Corollary 6. Taking ζ (̊s,æ) = s̊−æ in Theorem (2), we derive the following inequality: §(æ) + §(̊s) 2 Jαβ,γ(ω; p)− 1 2(̊s− æ)β−1 × [( Jæ + æ+ζ (̊s,æ),β−1 ) ( ω′, § ) + ( J (æ+ζ (̊s,æ))− æ,β−1 ) ( ω′, § )] ≤ (̊s− æ) 2 (∣∣§′(æ)∣∣+ ∣∣§′(̊s)∣∣) ∫ 1 0 +∞∑ n=0 ∣∣∣∣ (γ)n Γ(βn+ α) wn n! ∣∣∣∣ × ∣∣∣∣(1− to) β+αn−1 − (to) β+αn−1 h(to) ∣∣∣∣ dto. Theorem 3. Consider the function § : I = [æ,æ+ζ (̊s,æ)] −→ (0,+∞), where I ∈ R, and assume it is differentiable on I. Additionally, let |§′|q be an h-Godunova-Levin preinvex function on I, with p > 1 and q = p p−1 ; then.∣∣∣∣ §(æ) + §(æ + ζ (̊s,æ)) 2 Jαβ,γ(ω; p)− 1 2ζ (̊s,æ)β−1 × [( ℑæ+ æ+ζ (̊s,æ),β−1 ) ( ω′, § ) + ( ℑ(æ+ζ (̊s,æ))− æ,β−1 ) ( ω′, § )] | R. S. Ali et al. / Eur. J. Pure Appl. Math, 18 (1) (2025), 5725 10 of 14 ≤ ζ (̊s,æ) 2 (∣∣§′(æ)∣∣q + ∣∣§′(̊s)∣∣q)1/q × (∫ 1 0 ∣∣∣(1− to) β−1Jαβ,γ (ω(1− to) α; p)− (to) β−1Jαβ,γ (ω(to) α; p) ∣∣∣p dto)1/p × (∫ 1 0 1 h(to) dto )1/q . Proof. Using Lemma 1, we have:∣∣∣∣ §(æ) + §(æ + ζ (̊s,æ)) 2 Jαβ,γ(ω; p)− 1 2ζ (̊s,æ)β−1 × [( ℑæ+ æ+ζ (̊s,æ),β−1 ) ( ω′, § ) + ( ℑ(æ+ζ (̊s,æ))− æ,β−1 ) ( ω′, § )] | = ∣∣∣∣ζ (̊s,æ)2 I ∣∣∣∣ ≤ ζ (̊s,æ) 2 ∫ 1 0 ∣∣∣(1− to) β−1Jαβ,γ (ω(1− to) α; p)− (to) β−1Jαβ,γ (ω(to) α; p) ∣∣∣ × ∣∣§′(æ + toζ (̊s,æ)) ∣∣dto. Using Holder integral inequality, we have ≤ ζ (̊s,æ) 2 (∫ 1 0 ∣∣∣(1− to) β−1Jαβ,γ (ω(1− to) α; p)− (to) β−1Jαβ,γ (ω(to) α; p) ∣∣∣p dto)1/p × (∫ 1 0 ∣∣§′(æ + toζ (̊s,æ)) ∣∣q dto)1/q . (11) Since (1/p) + (1/q) = 1, and because |§′|q is an (h-GL) preinvex function, we obtain:∫ 1 0 ∣∣§′(æ + toζ (̊s,æ)) ∣∣q dto ≤ ∫ 1 0 ( |§′(æ)|q h(to) + |§′(̊s)|q h(1− to) ) dto ≤ (∣∣§′(æ)∣∣q + ∣∣§′(̊s)∣∣q) ∫ 1 0 1 h(to) dto. (12) Using (12) in (11), we have the required result. Theorem 4. With the assumptions of Theorem 3, we get the following inequality related to the Hermite-Hadamard inequality:∣∣∣∣§(æ) + §(æ + ζ (̊s,æ)) 2 Jαβ,γ(ω; p)− 1 2ζ (̊s,æ)β−1 × [( ℑæ+ æ+ζ (̊s,æ),β−1 ) ( ω′, § ) + ( ℑ(æ+ζ (̊s,æ))− æ,β−1 ) ( ω′, § )] ≤ ζ (̊s,æ) 21/q (∣∣§′(æ)∣∣q + ∣∣§′(̊s)∣∣q)1/q [Jαβ,γ(ω; p)− ( 1 2 )β−1 Jαβ,γ ( ω ( 1 2 )α ; p )]1−(1/q) R. S. Ali et al. / Eur. J. Pure Appl. Math, 18 (1) (2025), 5725 11 of 14 × ∫ 1 0 ∣∣∣(1− to) β−1Jαβ,γ (ω(1− to) α; p)− (to) β−1Jαβ,γ (ω(to) α; p) ∣∣∣ h(to) dto  1 q . where β, α ∈ R+. Proof. According to Lemma 1, we have∣∣∣∣ §(æ) + §(æ + ζ (̊s,æ)) 2 Jαβ,γ(ω; p)− 1 2ζ (̊s,æ)β−1 × [( ℑæ+ æ+ζ (̊s,æ),β−1 ) ( ω′, § ) + ( ℑ(æ+ζ (̊s,æ))− æ,β−1 ) ( ω′, § )] | = ∣∣∣∣ζ (̊s,æ)2 I ∣∣∣∣ ≤ ζ (̊s,æ) 2 ∫ 1 0 ∣∣∣(1− to) β−1Jαβ,γ (ω(1− to) α; p)− (to) β−1Jαβ,γ (ω(to) α; p) ∣∣∣ ∣∣§′(æ + toζ (̊s,æ)) ∣∣dto Applying the power mean inequality, we derive:∣∣∣∣ §(æ) + §(æ + ζ (̊s,æ)) 2 Jαβ,γ(ω; p) − 1 2ζ (̊s,æ)β [( Jæ + æ+ζ (̊s,æ),β−1 ) ( ω′, § ) + ( J (æ+ζ (̊s,æ))− æ,β−1 ) ( ω′, § )]∣∣∣∣ ≤ ζ (̊s,æ) 2 (∫ 1 0 ∣∣∣(1− to) β−1Jαβ,γ (ω(1− to) α; p)− (to) β−1Jαβ,γ (ω(to) α; p) ∣∣∣dto)1−(1/q) × (∫ 1 0 ∣∣∣(1− to) β−1Jαβ+1,γ (ω(1− to) α; p)− (to) β−1Jαβ+1,γ (ω(to) α; p) ∣∣∣ × ∣∣§′(æ + toζ (̊s,æ)) ∣∣q dto )1/q . Since |§′|q is (h-GL) preinvex, we have∫ 1 0 ∣∣∣(1− to) β−1Jαβ,γ (ω(1− to) α; p)− (to) β−1Jαβ,γ (ω(to) α; p) ∣∣∣ ∣∣§′(æ + toζ (̊s,æ)) ∣∣q dto ≤ ∫ 1 0 ∣∣∣(1− to) β−1Jαβ,γ (ω(1− to) α; p)− (to) β−1Jαβ,γ (ω(to) α; p) ∣∣∣ h(to) ∣∣§′(æ)∣∣q dto + ∫ 1 0 ∣∣∣(1− to) β−1Jαβ,γ (ω(1− to) α; p)− (to) β−1Jαβ,γ (ω(to) α; p) ∣∣∣ h(1− to) ∣∣§′(̊s)∣∣q dto = (∣∣§′(æ)∣∣q + ∣∣§′(̊s)∣∣q) ∫ 1 0 ∣∣∣(1− to) β−1Jαβ,γ (ω(1− to) α; p)− (to) β−1Jαβ,γ (ω(to) α; p) ∣∣∣ h(to) dto. R. S. Ali et al. / Eur. J. Pure Appl. Math, 18 (1) (2025), 5725 12 of 14 Now consider, ∫ 1 0 ∣∣∣(1− to) βJαβ,γ (ω(1− to) α; p)− (to) βJαβ,γ (ω(to) α; p) ∣∣∣ dto = +∞∑ n=0 ∣∣∣∣ (γ)n Γ(βn+ α) wn n! ∣∣∣∣ ∫ 1 0 ∣∣∣(1− to) β+αs̊−1 − (to) β+αs̊−1 ∣∣∣ dto = +∞∑ n=0 ∣∣∣∣ (γ)n Γ(βn+ α) wn n! ∣∣∣∣ × [∫ 1/2 0 ∣∣∣(1− to) β+αs̊−1 − (to) β+αs̊−1 ∣∣∣dto + ∫ 1 1/2 ∣∣∣(1− to) β+αs̊−1 − (to) β+αs̊−1 ∣∣∣dto] = 2 [ Jαβ+1,γ(ω; p)− ( 1 2 )β−1 Jαβ+1,γ ( ω ( 1 2 )α ; p )] . 5. Conclusion In this work, we discussed the refinements of some well known inequalities for different convexity through prabhaker fractional operators. Using the Prabhakar fractional integral operators, Hermite-Hadamard fractional inequalities and trapezoidal inequalities for h Go- dunova Levin convex and preinvex functions are developed. To obtained some other well known inequalities, and presented in the form of corollaries, which shows the straightened of our main results. Various fractional versions of other recognized inequalities can be derived for h-Godunova-Levin convex and preinvex functions, contributing to significant advancements in the theory of fractional inequalities. Acknowledgements The authors A. Aloqaily, and N. Mlaiki would like to thank Prince Sultan University for paying the publication fees for this work through TAS. References [1] Thabet Abdeljawad and Dumitru Baleanu. Monotonicity results for fractional differ- ence operators with discrete exponential kernels. 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