International Journal of Analysis and Applications Volume 17, Number 3 (2019), 388-395 URL: https://doi.org/10.28924/2291-8639 DOI: 10.28924/2291-8639-17-2019-388 SOME PROPERTIES OF GEODESIC STRONGLY E-B-VEX FUNCTIONS WEDAD SALEH∗ Department of Mathematics, Taibah University, Al- Medina, Saudi Arabia ∗Corresponding author: wed 10 777@hotmail.com Abstract. Geodesic E-b-vex sets and geodesic E-b-vex functions on a Riemannian manifold are extended to the so called geodesic strongly E-b-vex sets and geodesic strongly E-b-vex functions. Some basic properties of geodesic strongly E-b-vex sets are also studied. 1. Introduction Convexity and its generalizations play an important role in optimization theory, convex anlysis and Minkowski space [3, 4, 6, 9, 10]. Youness [17] defined E-convex sets and E-convex functions by relaxing the definitions of convex sets and convex functions, which have some important applications in various branches of mathematical sci- ences [1, 12, 13]. Also, Youness [18] extended the definitions of E-convex sets and E-convex functions to strongly E-convex sets and strongly E-convex functions. The B-vex functions which shares many properties with convex functions was introduced by Bector and Singh [2]. Some reserchers studied some new gen- eralizations of convex functions by relaxing definitions of E-convex functions and B-vex functions such as E-B-vex functions [15] and strongly E-B-vex functions [19]. Also, generalization of convexity on Riemannian manifolds were presented in ( [5], [8] , [14], [16]). Received 2019-03-08; accepted 2019-04-05; published 2019-05-01. 2010 Mathematics Subject Classification. 52A20, 52A41, 53C20, 53C22. Key words and phrases. geodesic E-convex sets; geodesic E-convex functions; Riemannian manifolds. c©2019 Authors retain the copyrights of their papers, and all open access articles are distributed under the terms of the Creative Commons Attribution License. 388 https://doi.org/10.28924/2291-8639 https://doi.org/10.28924/2291-8639-17-2019-388 Int. J. Anal. Appl. 17 (3) (2019) 389 In this paper, a new class of sets on Riemannian manifolds, called geodesic strongly E-b-vex sets, and a new class of functions defined on them, called geodesic strongly E-convex functions, have been proposed. Also, some of their properties have been discussed. This paper divides into three sections. In section 2, some of definities and properties which will be used throughout this work are presented that can be found in many books on differential geometry such as [16] . In section 3, a geodedic strongly E-b-vex set and geodesic strongly E-b-vex function are studied with some of their properties. 2. Preliminaries Now, let ℵ is a C∞ n-dimensional Riemannian manifold, also µ1,µ2 ∈ℵ and δ : [0, 1] −→ℵ be a geodesic joining the points µ1 and µ2 , which means that δµ1,µ2 (0) = µ2 and δµ1,µ2 (1) = µ1. Strongly E-convex sets (SEC) and strongly E-convex (SEC) functions were introduced in [18] such as: Definition 2.1. (1) A subset Ω ⊆ Rn is strongly E-convex (SEC) set if there is a map ε: Rn −→ Rn such that δ(αµ1 + ε(µ1)) + (1 − δ)(αµ2 + ε(µ2)) ∈ B for each µ1,µ2 ∈ Ω,α ∈ [0, 1] and δ ∈ [0, 1]. (2) A function g : Ω ⊆ Rn −→ R is strongly E-convex (SEC) function on Ω if there is a map ε: Rn −→ Rn such that Ω is a SEC set and g(δ(αµ1 + ε(µ1)) + (1 −δ)(αµ2 + ε(µ2))) ≤ δg(ε(µ1)) + (1 − δ)g(ε(µ2)), ∀µ1,µ2 ∈ Ω,α ∈ [0, 1] and δ ∈ [0, 1]. Definition 2.2. [5] (1) Considering ε: ℵ −→ ℵ is a map. A subset Ω ⊂ ℵ is geodesic E-convex iff there exists a unique geodesic ηε(µ1),ε(µ2)(δ) of length d(µ1,µ2), which belongs to Ω, ∀µ1,µ2 ∈ Ω and δ ∈ [0, 1]. (2) A functin g : Ω ⊆ℵ−→ R where Ω is a GEC set in ℵ is geodesic E-convex if g(ηε(µ1),ε(µ2)(δ)) ≤ δg(ε(µ1)) + (1 − δ)g(ε(µ2)), ∀µ1,µ2 ∈ Ω and δ ∈ [0, 1]. Definition 2.3. [7] (1) Considering ε: ℵ −→ ℵ is a map. A subset Ω ⊂ ℵ is geodesic strongly E-convex(GSEC) iff there exists a unique geodesic ηαµ1+ε(µ1),αµ2+ε(µ2)(δ) of length d(µ1,µ2), which belongs to Ω, ∀µ1,µ2 ∈ Ω, α ∈ [0, 1] and δ ∈ [0, 1] and . Int. J. Anal. Appl. 17 (3) (2019) 390 (2) A functin g : Ω ⊆ ℵ −→ R, where Ω is a GSEC set in ℵ, is geodesic strongly E-convex (GSEC) funtion if g(ηαµ1+ε(µ1),αµ2+ε(µ2)(δ)) ≤ δg(ε(µ1)) + (1 −δ)g(ε(µ2)), ∀µ1,µ2 ∈ Ω and δ ∈ [0, 1]. 3. Geodesic Strongly E-b-vex Sets and Geodesic Strongly E-b-vex Functions In this part of work, a geodesic strongly E-b-vex (GSE-b-vex) set and a geodesic strongly E-b-convex (GSE-b-vex) function in a Riemannian manifold ℵ are given and some of their properties are discussed. Definition 3.1. A subset Ω of ℵ is called a geodesic strongly E-b-vex (GSE-b-vex) iff there exists a unique geodesic ηαµ1+ε(µ1),αµ2+ε(µ2)(δb) of length d(µ1,µ2), which belongs to Ω, ∀µ1,µ2 ∈ Ω,α ∈ [0, 1] and δ ∈ [0, 1]. Remark 3.1. (1) Every GSE-b-vex set is a GSEC set when b(µ1,µ2,δ) = 1. (2) Every GSE-b-vex set is a GE-b-vex set when α = 0. (3) When ηαµ1+ε(µ1),αµ2+ε(µ2)(δb) = δb (αµ1 + ε(µ1)) + (1 −δb) (αµ2 + ε(µ2)) , then we have strongly E-B-vex set. Now, some propertie of GSE-b-vex sets are propoed. Proposition 3.1. Every convex set Ω ⊂ℵ is a GSE-b-vex set. The proof of the above proposition is direct that by taking ε: ℵ−→ℵ as the identity map,b(µ1,µ2,δ) = 1 and α = 0. Proposition 3.2. Let Ω ⊂ℵ be a GSE-b-vex set, then ε(Ω) ⊆ Ω. Proof. Since Ω is a GSE-b-vex set, then ηαµ1+ε(µ1),αµ2+ε(µ2)(δb) ∈ Ω, µ1,µ2 ∈ Ω, α ∈ [0, 1] and δ ∈ [0, 1]. Let δb = 1 and α = 0, then ηε(µ1),ε(µ2) = ε(µ2) ∈ Ω, then ε(Ω) ⊆ Ω. � Theorem 3.1. Suppose that a set {Ωj}j=1,2,··· ,n is an arbitrary collection of GSE-v-vex subsets of ℵ, then ∩j=1,2,··· ,nΩi is a GSE-b-vex set. Proof. Considering {Ωj}j=1,2,··· ,n is a collection of GSE-b-vex subsets of Ω. If ∩j=1,2,··· ,nΩj is an empty set, then the result is obvious. Assume that µ1,µ2 ∈∩j=1,2,··· ,nΩj, then µ1,µ2 ∈ Ωj. Hence, ηαµ1+ε(µ1),αµ2+ε(µ2)(δb) ∈ Ωj,∀α ∈ [0, 1] and δ ∈ [0, 1]. Hence, ηαµ1+ε(µ1),αµ2+ε(µ2)(δb) ∈∩j=1,2,··· ,nΩj,∀α ∈ [0, 1] and δ ∈ [0, 1]. � Int. J. Anal. Appl. 17 (3) (2019) 391 Remark 3.2. However, the above theorem is not true for the union of GSE-b-vex sets. Now, we introduce the definition of a geodesic E-b-vex (GSE-b-vex) function on ℵ. Definition 3.2. Assume that Ω ⊂ℵ is a GSE-b-vex set . A function g : Ω −→ R is called a geodesic strongly E-b-vex (GSE-b-vex) if g(ηαµ1+ε(µ1),αµ2+ε(µ2)(δb)) ≤ γg(ε(µ1)) + (1 −γ)g(ε(µ2)), (3.1) ∀µ1,µ2 ∈ Ω,α ∈ [0, 1] and δ ∈ [0, 1]. If the inequality (3.1) is strict, then g is called a strictly GSE-b-vex function. Example 3.1. Assume that g : R −→ R such that g(µ) = −|µ|. Aslo, assume that ε: R −→ R is defined as ε(µ) = αµ where 0 < α ≤ 1,∀µ ∈ R and the geodesic η is given as ηαµ1+ε(µ1),αµ2+ε(µ2)(δb) =   1 2α [αµ2 + ε(µ2) + δb(αµ1 + ε(µ1) −αµ2 −ε(µ2))] ; µ1µ2 ≥ 0, 1 2α [αµ2 + ε(µ2) + δb(αµ2 + ε(µ2) −αµ1 −ε(µ1))] ; µ1µ2 < 0 =   µ2 + δb(µ1 −µ2) ; µ1µ2 ≥ 0, µ2 + δb(µ2 −µ1) ; µ1µ2 < 0, then g is GSE-b-vex function. Proposition 3.3. Let g : Ω −→ R be a GSE-b-vex function on a GSE-b-vex set Ω ×ℵ, then g(αµ + ε(µ)) ≤ g(ε(µ)), µ ∈ Ω and α ∈ [0, 1]. Proof. Since g is GSE-b-vex function on GSE-b-vex set Ω, then g(ηαµ1+ε(µ1),αµ2+ε(µ2)(δb)) ≤ δbg(ε(µ1)) + (1 −δb)g(ε(µ2)), then for δb = 1, we have g(αµ1 + ε(µ1)) ≤ g(ε(µ1)). � Theorem 3.2. If g1 : Ω −→ R is a GSE-b-vex function on a GSE-b-vex set Ω ⊂ ℵ and g2 : U −→ R is a non-decreasing convex function such that rang(g1) ⊂ U, then the composite function g2og1 is GSE-b-vex function on Ω. Int. J. Anal. Appl. 17 (3) (2019) 392 Proof. By using the hypothesis, we can write all x1,x2 ∈ B,α ∈ [0, 1] and γ ∈ [0, 1], g1(ηαµ1+ε(µ1),αµ2+ε(µ2)(δb)) ≤ δbg1(ε(µ1)) + (1 −δb)g1(ε(µ2)), ∀µ1,µ2 ∈ Ω,α ∈ [0, 1] and δ ∈ [0, 1] and since g2 is a non-decreasing convex function, then we get g2og1(ηαµ1+ε(µ1),αµ2+ε(µ2)(δb)) = g2 ( g2(ηαµ1+ε(µ1),αµ2+ε(µ2)(δb)) ) ≤ g2 (δbg1(ε(µ1)) + (1 −δb)g1(ε(µ2))) ≤ δbg2 (g1(ε(µ1))) + (1 − δb)g2 (g1(ε(µ2))) = δb(g2og1)(ε(µ1)) + (1 −δb)(g2og1)(ε(µ2)) hence, g2og1 is GSE-b-vex on Ω. Moreover, g2og1 is a strictly GSE-b-vex function if g2 is a strictly non- decreasing convex function. � Theorem 3.3. Considering gi : Ω −→ R, i = 1, 2, ...,n are GSE-b-vex functions. Then, the function g = n∑ i=1 ξigi is also GSE-b-vex geodesic on Ω, ∀ξi ∈ R,ξi ≥ 0. Proof. Since gi, i = 1, 2, ...,n are GSE-b-vex functions, then gi(ηαµ1+ε(µ1),αµ2+ε(µ2)(δb)) ≤ δbgi(ε(µ1)) + (1 − δb)gi(ε(µ2)), ∀µ1,µ2 ∈ Ω,α ∈ [0, 1] and δ ∈ [0, 1], Hence, ξigi(ηαµ1+ε(µ1),αµ2+ε(µ2)(δb)) ≤ δbξigi(ε(µ1)) + (1 − δb)ξigi(ε(µ2)). This implies to, g(ηαµ1+ε(x1),αµ2+ε(µ2)(δb)) = n∑ i=1 ξigi(ηαµ1+ε(x1),αµ2+ε(µ2)(δb)) ≤ δb n∑ i=1 ξigi(ε(µ1)) + (1 − δb) n∑ i=1 ξigi(ε(µ2)) = δbg(ε(µ1)) + (1 − δb)g(ε(µ2)). Then g is GSE-b-vex function. � Next, we show that a funcion is GSE-b-vex iff its epigraph is a GSE-b-vex set. Definition 3.3. Assume that Ω ⊂ ℵ× R,E : ℵ −→ ℵ, b : Ω × Ω × [0, 1] −→ R+ and F : R −→ R. A set Ω is called a geodesic strongly E ×F -convex ( GSE ×F -b-vex ) if ( ηαµ1+ε(µ1),αµ2+ε(µ2)(δb),δbF(ξ1) + (1 −δb)F(ξ2) ) ∈ Ω, ∀(µ1,ξ1), (µ2,ξ2) ∈ Ω, α ∈ [0, 1] and γ ∈ [0, 1]. Int. J. Anal. Appl. 17 (3) (2019) 393 Remark 3.3. From Definition 3.3, we have found Ω ⊆ℵ is a GSE-b-vex set iff Ω×R is a GSE×F -b-vex set. Now , the epigraph of a function g : Ω ⊂ℵ−→ R is given as E(g) = {(µ,a) : µ ∈ Ω,a ∈ R,g(µ) ≤ a} . (3.2) Theorem 3.4. Suppose that Ω ⊆ℵ is a GSE-b-vex set, g : Ω −→ R is a function and F : R −→ R is a map such that F(g(µ)+a) = g(ε(µ))+a, ∀a ∈ R, a > 0. Then, g is a GSE-b-vex on Ω iff E(g) is a GSE×F -b-vex on Ω ×R. Proof. Let (µ1,a1), (µ2,a2) ∈ E(g). Since Ω is GSE-b-vex, then ηαµ1+ε(µ1),αµ2+ε(µ2)(δb) ∈ Ω, ∀α ∈ [0, 1] and δ ∈ [0, 1]. When α = 0 and δb = 1, we have ε(µ1) ∈ Ω also, when α = 0 and δb = 0 we get ε(µ2) ∈ Ω. Assume that F(a1) and F(a2) where g(ε(µ1)) ≤ F(a1) and g(ε(µ2)) ≤ F(a2). Then (ε(µ1),F(a1)), (ε(µ2),F(a2)) ∈ E(g). Considering g is a GSE-b-vex on Ω, then g(ηαµ1+ε(µ1),αµ2+ε(µ2)(δb)) ≤ δbg(ε(µ1)) + (1 −δb)g(ε(µ2)) ≤ δbF(a1) + (1 − δb)F(a2). This is leading to, ( ηαµ1+ε(µ1),αµ2+ε(µ2)(δb),δbF(a1) + (1 − δb)F(a2) ) ∈ E(g), which means that E(g) is GSE × É-b-vex on Ω ×R. Conversely, let us take E(g) is GSE × É-b-vex on Ω × R. Assume that µ1,µ2 ∈ Ω,α ∈ [0, 1] and δ ∈ [0, 1], then (µ1,g(µ1)) ∈ E(g) and (µ2,g(µ2)) ∈ E(g). In addition, ( ηαµ1+ε(µ1),αµ2+ε(µ2)(δb),δbF(g(µ1)) + (1 − δb)F(g(µ2)) ) ∈ E(g) =⇒ g(ηαµ1+ε(µ1),αµ2+ε(µ2)(δb)) ≤ δbF(g(µ1)) + (1 −δb)F(g(µ2)) = δbg(ε(µ1)) + (1 − δb)g(ε(µ2)). Hence, the result. � Theorem 3.5. Let {Ωj}j=1,··· ,n be a family of GSE×F -b-vex sets. Then ∩j=1,··· ,nΩj is also GSE×F -b-vex set. Proof. Let (µ1,a1), (µ2,a2) ∈∩j=1,··· ,nΩj, then (µ1,a1), (µ2,a2) ∈ Ωj, ∀j. =⇒ ( ηαµ1+ε(µ1),αµ2+ε(µ2)(δb),δbF(a1) + (1 − δb)F(a2) ) ∈ Ωj, Int. J. Anal. Appl. 17 (3) (2019) 394 ∀α ∈ [0, 1] and δ ∈ [0, 1] . Hence, ( ηαµ1+ε(µ1),αµ2+ε(µ2)(δb),δbF(a1) + (1 − δb)F(a2) ) ∈∩j=1,··· ,nΩj, ∀α ∈ [0, 1] and δ ∈ [0, 1]. This shows that , ∩j=1,··· ,nΩj is GSE ×F-b-vex set. � Theorem 3.6. Suppose that G : R −→ R such that G(g(x) + µ) = g(ε(x)) + µ,∀µ ∈ R,µ > 0. Let {gi}i∈I be a family of real valued functions that is defined on a GSE-b-vex set Ω and bounded from above. Then, g(x) = supi∈Igi(x),x ∈ Ω is GSE-b-vex on Ω. Proof. Let gi, i ∈ I be a GSE-b-vex function on Ω, then E(gi) = {(x,µ) : x ∈ Ω,µ ∈ R,gi(x) ≤ µ} are GSE ×F-b-vex on Ω ×R. Hence, ∩i∈IE(gi) = {(x,µ) : x ∈ Ω,µ ∈ R,gi(x) ≤ µ,i ∈ I} = {(x,µ) : x ∈ Ω,µ ∈ R,g(x) ≤ µ} is GSE ×F-b-vex set. 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