EUROPEAN JOURNAL OF PURE AND APPLIED MATHEMATICS 2025, Vol. 18, Issue 3, Article Number 6349 ISSN 1307-5543 – ejpam.com Published by New York Business Global Fekete-Szegö Inequality Estimate for Analytic Functions Using Sǎlǎgean-Difference Operator and Leaf-Like Domain Avaya Naik1,∗, Sushree Chinmayee Sahoo1 1 P.G. Department of Mathematics Fakir Mohan University,Balasore, Odisha, India Abstract. This paper investigates the Fekete-Szegö inequality for subclasses of analytic func- tions in the unit disk, including starlike, convex, bounded turning, and close-to-convex functions of complex order. Employing the Sǎlǎgean-difference operator, we derive sharp bounds for the functional |b3−γb22| and extend these results to leaf-like domains. Our findings generalize classical inequalities, offering new insights into coefficient constraints and geometric properties in complex analysis. 2020 Mathematics Subject Classifications: 30C45 Key Words and Phrases: Analytic function, Univalent functions,Fekete-Szegö inequality,Leaf like domain 1. Introduction The theory of univalent functions, a cornerstone of geometric function theory, explores the properties of analytic functions that are injective in the open unit disk. A fundamental problem in this field is to estimate the coefficients of such functions, as these coefficients encode critical geometric and analytic information about their mappings. Among the clas- sical results, the Fekete-Szegö inequality stands out as a powerful tool for a normalized analytic function. The Fekete-Szegö inequality was first proposed by Hungarian Mathe- maticians Michael Fekete and Gaber Szegö in 1933 (see[1]). Since then, the various au- thors were investigated and obtained the Fekete-Szegö inequalities for different subclasses (see[2][3][4],[5],[6],[7],[8],[9],[10])This inequality has been extensively studied for various subclasses of univalent functions, such as starlike, convex, and close-to-convex functions, due to its applications in understanding extremal problems and conformal mappings. In recent decades, differential and integral operators have enriched the study of uni- valent functions by generalizing classical subclasses and introducing new geometric con- straints. One such operator is the Sǎlǎgeandifferential operator, introduced by Sǎlǎgean ∗Corresponding author. DOI: https://doi.org/10.29020/nybg.ejpam.v18i3.6349 Email addresses: avayanaik@gmail.com (A.Naik), chinmayee144@gmail.com (S. C. Sahoo) https://www.ejpam.com 1 Copyright: © 2025 The Author(s). (CC BY-NC 4.0) A.Naik, S. C. Sahoo / Eur. J. Pure Appl. Math, 18 (3) (2025), 6349 2 of 14 in 1983 (see[11]), which iteratively applies weighted combinations of the function and its derivatives to generate new classes of analytic functions. Building on this foundation, Al-Oboudi (see [12]) proposed a generalized difference operator, later adapted to form the Salagean-difference operator, denoted Dβ λ . Parallel to operator-based studies, the exploration of non-standard domains has gained traction in complex analysis.The leaf-like domains, defined by mappings exhibit unique boundary properties that deviate from the circular or convex shapes typically associated with starlike or convex functions. These domains, named for their resemblance to a leaf?s contour, challenge traditional coefficient bounds and inspire new inequalities tailored to their geometry. The interplay between differential operators and such domains is partic- ularly intriguing, as it allows researchers to investigate how operator-induced transforma- tions affect mappings onto complex regions. The research conducted by Srivastava et al.(see [13]),Murugusundaramoorthy (see [14]), Orhan and Cot̆irlă ([15] ), Al-Sadi (see[16]), Panigrahi et al.([17]) advances the the- oretical foundations of these subclasses. Several scholars, including Al-Sadi (see[16]) and Srivastava et al.(see [13]), focused on deriving constraints for the initial coefficients, which are crucial for understanding the evolution and structure of these functions. The Fekete- Szegö functional was the focus of several investigations, including those by Srivastava et al. (see [13]) and Panigrahi et al. (see[17]), which provided upper estimates and inequal- ities for these specialized subclasses. And the Geometric structures like leaf-shaped do- mains Panigrahi et al.(see[17]) and crescent-shaped areas Murugusundaramoorthy,(see[14]) demonstrate how these functions can be connected to specific geometric curves and figures, impacting their analytical behavior. Recently Kavita P et al.(see[18]) obtained significant inequality for starlike, bounded turning, and close-to-convex functions by using Hohlov operator and taking leaf like do- main in account. Motivated by these developments, this paper derives new Fekete-Szegöinequality esti- mates for subclasses of analytic functions defined using the Sǎlǎgean-difference operator Dβ λ and associated with leaf-like domains. Specifically, we consider functions in classes such as starlike, convex, bounded turning, and close-to-convex functions of complex order, extending classical results to these generalized settings. Our main objective is to obtain sharp bounds for the functional |b3−γb22| for functions h(ζ) satisfying Dβ λh(ζ) ∈ S∗ ℘ where S∗ ℘, denotes a starlike class relative to a specific subordination. Additionally, we explore how these bounds adapt to mappings onto leaf-like domains, offering insights into their geometric implications. The novelty of this work lies in its integration of the Sǎlǎgean-difference operator with leaf-like domains, a combination that has not been extensively studied in the context of the Fekete-Szegö problem. By leveraging known results on coefficient bounds (see [19][20]) and introducing new techniques for handling the operators symmetry, we establish inequalities that generalize and sharpen existing estimates. These findings not only enhance our understanding of univalent function behavior but also pave the way for applications in conformal mapping and operator theory. Let A be the family of function h which are analytic in the open unit dick ∆ = {ζ : A.Naik, S. C. Sahoo / Eur. J. Pure Appl. Math, 18 (3) (2025), 6349 3 of 14 |ζ| < 1} normalized by the conditions h(0) = 0 and h′(0) = 1 with the series expansion of the form h(ζ) = ζ + ∞∑ n=2 bnζ n (1) Let S be a subclass of A consists of ”schilit functions”. The sufficient conditions for a function h ∈ A to belong to the classes S∗ (starlike functions) and Sc (convex functions) are well established results in geometric function theory. These foundational conditions can be trace back to the pioneering contribution of W.odzimierz̀erański, Robertson, and Hummel in the mid-20th century. Alexander (see[21]) introduced the necessary and suffi- cient condition for a function h ∈ A to be in S∗ is that Re {ζh′(ζ) h(ζ) } > 0, (ζ ∈ ∆) Similarly, the necessary and sufficient condition for a function h ∈ A to be in Sc is that Re { 1 + ζh′′(ζ) h′(ζ) } > 0, (ζ ∈ ∆) In 1964, Robertson [22] introduced a generalized class of starlike and convex functions of complex order. Subsequently, Miller and Mocanu [23] incorporated similar conditions in their work to extend classical results related to starlike and convex functions. These condi- tions were formulated using differential subordinations, a powerful technique for analyzing functional inequalities within geometric function theory. These classes have been thoroughly examined, and various characteristics have been identified, such as coefficient bounds, growth and distortion theorems, radii of starlike- ness and convexity, as well as properties related to convolution, Hadamard products, and subordination. These functions facilitate the development of new function classes, aid in modeling intricate geometric forms, and contribute to a deeper understanding of geometric properties. Let α ∈ C, a function h ∈ A is in the class of starlike functions of complex order α and denoted by S∗(α), [24] if and only if h(ζ) ζ ̸= 0 and Re ( 1 + 1 α { ζh′(ζ) h(ζ) − 1 }) > 0, (ζ ∈ ∆) (2) A function h ∈ A is in the class of convex functions of complex order α and denoted by C(α),[25] if and only if h′(ζ) ̸= 0 and Re ( 1 + 1 α { ζh′′(ζ) h′(ζ) }) > 0, (ζ ∈ ∆) (3) A function h ∈ A is in the class of convex functions of complex order α and denoted by K(α),[25] if and only if Re ( 1 + 1 α (h′(ζ)− 1) ) > 0 (ζ ∈ ∆) (4) A.Naik, S. C. Sahoo / Eur. J. Pure Appl. Math, 18 (3) (2025), 6349 4 of 14 For a function h ∈ A the class of analytic functions with h(0) = 0 and h′(0) = 1, the operator is defined as Dβ λ : A −→ A as follows: D0 λh(ζ) = h(ζ) D1 λh(ζ) = ζh′(ζ) + λ 2 [h(ζ)− h(−ζ)− 2ζ] (λ ∈ R) = ζ + ∞∑ n=2 [ n+ λ 2 (1 + (−1)n+1) ] bnζ n D2 λh(ζ) = D1(D1 λh(ζ)) In general, for β ∈ N0 = {0, 1, 2, 3, · · · }, Dβ λh(ζ) = D1 λ(D β−1 λ h(ζ)) = ζ + ∞∑ n=2 [ n+ λ 2 (1 + (−1)n+1) ]β bnζ n (ζ ∈ ∆) (5) This operator, characterized by its parameter λ and β order offers a versatile framework for studying function behavior under symmetric transformations, bridging classical differential operators and modern geometric constraints. The Operator Dβ λ is known as the Sǎlǎgean- difference operator in literature (see [26],[27]). This operator is a modified Dunkel operator of complex variables(see [28],[29]). When λ = 0,Dλ = Dβ 0 = Dβ is known as the Sǎlǎgean- differential operator (see [11]). Example 1. h(ζ) = ζ + ζ2 2 + ζ3 8 + ζ4 48 + ζ5 384 + · · · Then D1 1h(ζ) = ζ + ζ2 + ζ3 2 + ζ4 12 + ζ5 64 + · · · Example 2. h(ζ) = ζ + 2ζ2 5 + 3ζ3 25 + 4ζ4 125 + · · · Then h(ζ) = ζ + 4ζ2 5 + 12ζ3 25 + 16ζ4 125 + · · · 2. Preliminaries Let us define the bounded turning function with Sǎlǎgean- difference operator as R℘ which contains all the function h ∈ A and satisfying Re ( (Dβ λh(ζ)) ′), (ζ ∈ ∆) (6) A.Naik, S. C. Sahoo / Eur. J. Pure Appl. Math, 18 (3) (2025), 6349 5 of 14 Similarly starlike function with Sǎlǎgean- difference operator S∗ ℘ which maps |∆| < 1 conformally on to starlike domain and statisfying Re ( ζ(Dβ λh(ζ)) ′ Dβ λh(ζ) ) (ζ ∈ ∆) (7) Let us define starlike function of complex order with Sǎlǎgean- difference operator S∗ ℘(α) which maps |∆| < 1 conformally onto starlike domain of complex order and satisfying Re ( 1 + 1 α [ ζ(Dβ λh(ζ)) ′ Dβ λh(ζ) − 1 ]) > 0 (ζ ∈ ∆) (8) Let us define convex function of complex order with Sǎlǎgean- difference operator Sc ℘(α), which maps |ζ| < 1 conformally onto convex domain of complex order and satisfying Re ( 1 + 1 α [ ζ(Dβ λh(ζ)) ′′ (Dβ λh(ζ)) ′ − 1 ]) > 0 (ζ ∈ ∆) (9) Let us define close to convex function with Sǎlǎgean- difference operator K℘(α), which maps |ζ| < 1 conformally onto closed convex domain of complex order and satisfying Re { 1 + 1 α [(Dβ λh(ζ)) ′ − 1] } , (ζ ∈ ∆) (10) Raina and Sokol [30] and Haripriya [31] explored the function h(ζ) = ζ + (1 + ζ3) 1 3 , which has symmetry with respect to the real axis. Real part of this function is positive with conditions h(0) = h′(0) = 1, and it maps the unit disc onto analytic and univalent region which has the shape of leaf-like domain.This leaf-like domain can model complex shapes with smooth boundaries. In general, a ”leaf” is a smooth submanifold or region of a manifold that resembles ”sheets” within a system with layers. Particular subsets, or ”leaves,” inside a manifold are referred to as leaf-like domains when discussing foliations or decompositions of the manifold into simpler structures. In certain geometric contexts, such as the study of dynamical systems or the theory of foliations, examining the behavior of the manifold within these leaves can provide crucial insights into the general topology and geometry of the space. The result of following Lemmas are applied in our main theorems. Lemma 1. Let P denote the class of function denoted by p such that p(ζ) = d1ζ + d2ζ 2+ d3ζ 3 + · · · be an analytic function in the region R with the property that p(0) = 1 then |dn| ≤ 2 for all n ≥ 1 and |d2 − d21 2 |. P is the class of all such function which has the property of positive real part. Lemma 2. Let the analytic function p(ζ) = d1ζ+d2ζ 2+d3ζ 3+ · · · which have the positive real part, then |d2 − αd21| ≤ 2max1, |2α− 1| here α is the complex number. Functions p(ζ) = 1+ζ2 1−ζ2 and p(ζ) = 1+ζ 1−ζ provides the sharp results. A.Naik, S. C. Sahoo / Eur. J. Pure Appl. Math, 18 (3) (2025), 6349 6 of 14 3. Main Results Theorem 1. If h ∈ A is the form given by (1) belongs S∗ ℘ and γ is a real number then |b3 − γb22| ≤  1 2(3+λ)β if p(ζ) = 1+ζ2 1−ζ2 1 2(3+λ)β ∣∣∣2γ(3+λ)β 22β − 1 ∣∣∣ if p(ζ) = 1+ζ2 1−ζ2 (11) Proof. If h ∈ S∗Mα , then for the schwarz function w with w(0) = 0 and |w(ζ)| ≤ 1 and concept of sub-ordination property of equation (7), we have ζ(Dβ λh(ζ)) ′ Dβ λh(ζ) = w(ζ) + 3 √ 1 + (w(ζ))3 (12) we have p(ζ) = 1 + w(ζ) 1− w(ζ) = 1 + d1ζ + d2ζ 2 + d3ζ 3 + · · · w(ζ) = 1 + p(ζ) 1− p(ζ) on simplifying right hand side of equation (25) we get w(ζ) + 3 √ 1 + (w(ζ))3 = 1 + d1 2 ζ + ( d2 2 − d21 4 ) ζ2 + ( d3 2 − d1d2 2 + d31 6 ) ζ3+ (13)( d4 2 − d22 4 − d1d3 2 + d21d2 2 − d41 8 ) ζ4 + · · · From left hand side of (25) we get ζ(Dβ λh ′(ζ)) Dβ λh(ζ) = 1 + 2βb2ζ + ( 2(3 + λ)βb3 − 22βb22 ) ζ2 + ( 3(4β)b4 − 3(2β)(3 + λ)βb2b3 + 23βb32 ) ζ3 (14) + ( 4(5 + λ)βb5 − 4(2β)4βb2b4 − 2(3 + λ)2βb23 − 24βb42 + 4(22β)(3 + λ)βb22b3 ) ζ4 + · · · Now from (12),(13) and (14) 1 + 2βb2ζ + ( 2(3 + λ)βb3 − 22βb22 ) ζ2 + ( 3(4β)b4 − 3(2β)(3 + λ)βb2b3 + 23βb32 ) ζ3 + ( 4(5 + λ)βb5 − 4(2β)4βb2b4 − 2(3 + λ)2βb23 − 24βb42 + 4(22β)(3 + λ)βb22b3 ) ζ4 + · · · = 1 + d1 2 ζ + ( d2 2 − d21 4 ) ζ2 + ( d3 2 − d1d2 2 + d31 6 ) ζ3+ A.Naik, S. C. Sahoo / Eur. J. Pure Appl. Math, 18 (3) (2025), 6349 7 of 14( d4 2 − d22 4 − d1d3 2 + d21d2 2 − d41 8 ) ζ4 + · · · On equating the coefficients, we get b2 = d1 2(2β) b3 = d2 4(3 + λ)β b3 − γb22 = 1 4(3 + λ)β ( d2 − γ(3 + λ)βd21 22β ) Applying the lemma (2) we get |b3 − γb22| ≤ 1 2(3 + λ)β max { 1, ∣∣∣∣2γ(3 + λ)β 22β ∣∣∣∣} (15) This Completes the proof Theorem 2. If h ∈ A is the form given by (1) belongs RM℘ and γ is a real number then |b3 − γb22| ≤  1 3(3+λ)β if p(ζ) = 1+ζ2 1−ζ2 1 3(3+λ)β ∣∣∣3γ(3+λ)β 4(2)2β ∣∣∣ if p(ζ) = 1+ζ2 1−ζ2 (16) Proof. If RM℘ , then for the schwarz function w with w(0) = 0 and |w(ζ)| ≤ 1 (Dβ λh(ζ)) ′ = w(ζ) + 3 √ 1 + (w(ζ))3 (17) (Dβ λh(ζ)) ′ = 1 + 2(2β)b2ζ + 3(3 + λ)βb3ζ 2 + 4(4β)b4ζ 3 + 5(5 + λ)βb5ζ 5 + · · · (18) From equation (13) and (18) we have 1 + 2(2β)b2ζ + 3(3 + λ)βb3ζ 2 + 4(4β)b4ζ 3 + 5(5 + λ)βb5ζ 5 + · · · = 1 + d1 2 ζ + ( d2 2 − d21 4 ) ζ2 + ( d3 2 − d1d2 2 + d31 6 ) ζ3+( d4 2 − d22 4 − d1d3 2 + d21d2 2 − d41 8 ) ζ4 + · · · On contrasting similar terms b2 = d1 4(2β) b3 = 1 3(3 + λ)β ( d2 2 − d21 4 ) A.Naik, S. C. Sahoo / Eur. J. Pure Appl. Math, 18 (3) (2025), 6349 8 of 14 on streamlining and using lemma (2) we get |b3 − γb22| ≤ 1 3(3 + λ)β max { 1, ∣∣∣∣3γ(3 + λ)β 4(22β) ∣∣∣∣} (19) Theorem 3. If h ∈ A is the form given by (1) belongs S∗M℘(α) and γ is a real number then |b3 − γb22| ≤  α 2(3+λ)β if p(ζ) = 1+ζ2 1−ζ2 α 2(3+λ)β ∣∣∣(2γ(3+λ)β 22β − 1 ) α ∣∣∣ if p(ζ) = 1+ζ2 1−ζ2 (20) Proof. 1 + 1 α ( ζ(Dβ λh(ζ)) ′ Dβ λh(ζ) − 1 ) = w(ζ) + 3 √ 1 + (w(ζ))3 (21) and 1 + 1 α ( ζ(Dβ λh(ζ)) ′ Dβ λh(ζ) − 1 ) (22) = 1 + 1 α [ 2βb2ζ + ( 2(3 + λ)βb3 − 22βb22 ) ζ2 + ( 3(4β)b4 − 3(2β)(3 + λ)βb2b3 + 23βb32 ) ζ3 + ( 4(5 + λ)βb5 − 4(2β)4βb2b4 − 2(3 + λ)2βb23 − 24βb42 + 4(22β)(3 + λ)βb22b3 ) ζ4 + · · · ] from equation (13),(21) and (22) 1 + 1 α [ 2βb2ζ + ( 2(3 + λ)βb3 − 22βb22 ) ζ2 + ( 3(4β)b4 − 3(2β)(3 + λ)βb2b3 + 23βb32 ) ζ3 + ( 4(5 + λ)βb5 − 4(2β)4βb2b4 − 2(3 + λ)2βb23 − 24βb42 + 4(22β)(3 + λ)βb22b3 ) ζ4 + · · · ] = 1 + d1 2 ζ + ( d2 2 − d21 4 ) ζ2 + ( d3 2 − d1d2 2 + d31 6 ) ζ3+( d4 2 − d22 4 − d1d3 2 + d21d2 2 − d41 8 ) ζ4 + · · · By equating the like term we have b2 = d1α 2(2β) b3 = α 4(3 + λ)β ( d2 − d21 2 (1− α) ) A.Naik, S. C. Sahoo / Eur. J. Pure Appl. Math, 18 (3) (2025), 6349 9 of 14 On simplifying by lemma (2) we get |b3 − γb22| ≤ α 2(3 + λ)β max { 1, ∣∣∣∣(2γ(3 + λ)β 22β − 1 ) α ∣∣∣∣} As a result, we get the desired outcomes. Theorem 4. If h ∈ A is the form given by (1) belongs KM℘ and γ is a real number then |b3 − γb22| ≤  α 3(3+λ)β if p(ζ) = 1+ζ2 1−ζ2 α 3(3+λ)β ∣∣∣3γα(3+λ)β 4(2)2β − 1 ∣∣∣ if p(ζ) = 1+ζ2 1−ζ2 Proof. If KM℘, then for the schwarz function w with w(0) = 0 and |w(ζ)| ≤ 1 1 + 1 α ( (Dβ λh(ζ)) ′ − 1 ) = w(ζ) + 3 √ 1 + (w(ζ))3 (23) 1+ 1 α ( (Dβ λh(ζ)) ′−1 ) = 1+ 1 α ( 2(2β)b2ζ+3(3+λ)βb3ζ 2+4(4β)b4ζ 3+5(5+λ)βb5ζ 5+ · · · ) (24) From equation (13),(23) and (24) 1 + 1 α ( 2(2β)b2ζ + 3(3 + λ)βb3ζ 2 + 4(4β)b4ζ 3 + 5(5 + λ)βb5ζ 5 + · · · ) = 1 + d1 2 ζ + ( d2 2 − d21 4 ) ζ2 + ( d3 2 − d1d2 2 + d31 6 ) ζ3+( d4 2 − d22 4 − d1d3 2 + d21d2 2 − d41 8 ) ζ4 + · · · On contrasting similar terms b2 = d1α 4(2β) b3 = α 6(3 + λ)β ( d2 − d21 2 ) on streamlining and using lemma (2) we get |b3 − γb22| ≤ α 3(3 + λ)β max { 1, ∣∣∣∣3γα(3 + λ)β 4(22β) ∣∣∣∣} As a result, we get the desired outcomes. A.Naik, S. C. Sahoo / Eur. J. Pure Appl. Math, 18 (3) (2025), 6349 10 of 14 Theorem 5. If h ∈ A is the form given by (1) belongs ScM℘(α) and γ is a real number then |b3 − γb22| ≤  α 6(3+λ)β if p(ζ) = 1+ζ2 1−ζ2 α 6(3+λ)β ∣∣∣3γα(3+λ)β 2(22β) − α ∣∣∣ if p(ζ) = 1+ζ2 1−ζ2 (25) Proof. 1 + 1 α ( ζ(Dβ λh(ζ)) ′′ (Dβ λh(ζ)) ′ ) = w(ζ) + 3 √ 1 + (w(ζ))3 (26) and 1 + 1 α ( ζ(Dβ λh(ζ)) ′′ (Dβ λh(ζ)) ′ ) = (27) 1 + 1 α [ 2(2β)b2ζ + ( 6(3 + λ)βb3 − 4(22β)b22 ) ζ2+( 12(4β)a4 − 18(2β)(3 + λ)βb2b3 + 8(23β)b32 ) ζ3 + · · · ] From equation (13),(26) and (27), we have b2 = d1α 4(2β) b3 = α 6(3 + λ)β ( d2 2 − d21 4 (1− α) ) On simplifying by lemma (2) we get |b3 − γb22| ≤ α 6(3 + λ)β max { 1, ∣∣∣∣(3γα(3 + λ)β 2(22β) − α )∣∣∣∣} As a result, we get the desired outcomes. Remark 1. case-I: If p(ζ) = 1+ζ 1−ζ then in this case d1 = d2 = d3 = · · · = 2. Case-II: If p(ζ) = 1+ζ2 1−ζ2 then in this case d1 = d3 = d5 = · · · = 0 and d2 = d4 = d6 = · · · = 2. On taking consideration of these above instance we get the results of above theorems. 4. special cases Remark 2. If we take λ = 0 in Dβ λh(ζ), it will reduce to Sǎlǎgean-deferential Operator and ,β = 1 then 2β = 2, 1 (3+λ)β = 1 3 so that in theorem (1),(2),(3),(4),(5) we find the coresponding results of Sǎlǎgean deference Operator. A.Naik, S. C. Sahoo / Eur. J. Pure Appl. Math, 18 (3) (2025), 6349 11 of 14 Corollary 1. Let λ = 0, β = 1 , If h ∈ S∗M℘, then |b3 − γb22| ≤  1 6 if p(ζ) = 1+ζ2 1−ζ2 1 6 ∣∣∣3γ2 − 1 ∣∣∣ if p(ζ) = 1+ζ2 1−ζ2 Corollary 2. Let λ = 0, β = 1 , If h ∈ RM℘, then |b3 − γb22| ≤  1 9 if p(ζ) = 1+ζ2 1−ζ2 1 9 ∣∣∣9γ16 ∣∣∣ if p(ζ) = 1+ζ2 1−ζ2 Corollary 3. Let λ = 0, β = 1 , If h ∈ S∗M℘(α), then |b3 − γb22| ≤  α 6 if p(ζ) = 1+ζ2 1−ζ2 α 6 ∣∣∣(3γ 2 − 1 ) α ∣∣∣ if p(ζ) = 1+ζ2 1−ζ2 Corollary 4. Let λ = 0, β = 1 , If h ∈ KM℘(α), then |b3 − γb22| ≤  α 9 if p(ζ) = 1+ζ2 1−ζ2 α 9 ∣∣∣9γα16 − 1 ∣∣∣ if p(ζ) = 1+ζ2 1−ζ2 Corollary 5. Let λ = 0, β = 1 . If h ∈ ScM℘(α), then |b3 − γb22| ≤  α 18 if p(ζ) = 1+ζ2 1−ζ2 α 18 ∣∣∣9γα8 − α ∣∣∣ if p(ζ) = 1+ζ2 1−ζ2 Remark 3. If we take λ = 1, in Dβ λh(ζ) then it will reduce to Al-Oboudi differential operator, β = 1 then 2β = 2 and 1 (3+λ)β = 1 4 so that in theorem (1), (2), (3), (4), (5) we find the coresponding results of Al-Oboudi differential operator. Corollary 6. Let λ = 1, β = 1 , If h ∈ S∗M℘, then |b3 − γb22| ≤ { 1 8 if p(ζ) = 1+ζ2 1−ζ2 1 8 ∣∣2γ − 1 ∣∣ if p(ζ) = 1+ζ2 1−ζ2 Corollary 7. Let λ = 1, β = 1 , If h ∈ RM℘, then |b3 − γb22| ≤  1 12 if p(ζ) = 1+ζ2 1−ζ2 1 12 ∣∣∣3γ4 ∣∣∣ if p(ζ) = 1+ζ2 1−ζ2 Corollary 8. Let λ = 1, β = 1 , If h ∈ S∗M℘(α), then |b3 − γb22| ≤ { α 8 if p(ζ) = 1+ζ2 1−ζ2 α 8 ∣∣(2γ − 1)α ∣∣ if p(ζ) = 1+ζ2 1−ζ2 A.Naik, S. C. Sahoo / Eur. J. Pure Appl. Math, 18 (3) (2025), 6349 12 of 14 Corollary 9. Let λ = 1, β = 1 , If h ∈ KM℘(α), then |b3 − γb22| ≤  α 12 if p(ζ) = 1+ζ2 1−ζ2 α 12 ∣∣∣3γα4 − 1 ∣∣∣ if p(ζ) = 1+ζ2 1−ζ2 Corollary 10. Let λ = 1, β = 1 . If h ∈ ScM℘(α), then |b3 − γb22| ≤  α 24 if p(ζ) = 1+ζ2 1−ζ2 α 24 ∣∣∣3γα2 − α ∣∣∣ if p(ζ) = 1+ζ2 1−ζ2 5. Conclusion In conclusion, this work expands our understanding of the Fekete-Szegö inequality by applying it to a larger class of holomorphic functions, specifically starlike, bounded turning, and close-to-convex functions of complex order. By considering the Sǎlǎgean- difference operator and leaf-like domains, we have created new inequalities that expand on conventional findings. These findings improve our understanding of how these functions behave in geometric function theory and complex analysis.Additionally, we examine spe- cific instances of the deferential operator and provide strict limitations on the coefficients, providing useful information for further study. Acknowledgements The authors would like to express sincere gratitude to the editorial board and anony- mous reviewers of the European Journal of Pure and Applied Mathematics for their valu- able comments and suggestions, which helped to improve the quality and clarity of this research article. 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