2_dorca.dvi EUROPEAN JOURNAL OF PURE AND APPLIED MATHEMATICS Vol. 6, No. 1, 2013, 11-19 ISSN 1307-5543 – www.ejpam.com Mapping Properties of Some Classes of Analytic Functions Under New Generalized Integral Operators Irina Dorca1,∗, Daniel V. Breaz 2 1 Department of Mathematics, University of Piteşti, Argeş, România 2 Department of Mathematics, University "1st December 1918" of Alba, România Abstract. In this paper we study the mapping properties with respect to new generalised integral operator which was studied recently. 2010 Mathematics Subject Classifications: 30C45 Key Words and Phrases: analytic functions, positive coefficients, negative coefficients, integral oper- ator 1. Introduction LetH (U) be the set of functions which are regular in the unit disc U , A = { f ∈H (U) : f (0) = f ′(0)− 1= 0} and S = { f ∈A : f is univalent in U}. In [10] the subfamily T of S consisting of functions f of the form f (z) = z − ∞ ∑ j=2 a jz j , a j ≥ 0, j = 2,3, . . . , z ∈ U (1) was introduced. Thus we have the subfamily S − T consisting of functions f of the form f (z) = z + ∞ ∑ j=2 a jz j , a j ≥ 0, j = 2,3, . . . , z ∈ U (2) ∗Corresponding author. Email addresses: irina.dor a�gmail. om (I. Dorca), dbreaz�uab.ro (D. Breaz) http://www.ejpam.com 11 c© 2013 EJPAM All rights reserved. I. Dorca, D. Breaz / Eur. J. Pure Appl. Math, 6 (2013), 11-19 12 A function f (z) ∈ A is said to be spiral-like if there exists a real number λ, |λ| < π/2, such that Re eiλ z f ′(x) f (X ) , (z ∈ U). The class of all spiral-like functions was introduced by L. Spacek [11] and we denote it by S⋆ λ . Later, Robertson [9] considered the class Cλ of analytic functions in U for which z f ′(z) ∈ S⋆ λ . Let Pλ k (ρ) be the class of functions p(z) analytic in U with p(0) = 1 and 2π ∫ 0 � � � � � Re eiλp(z)−ρ cosλ 1−ρ � � � � � dθ ≤ kπ cosλ, z = reiθ (3) where k ≥ 2, 0 ≤ ρ < 1, λ is real with |λ| < π 2 . In case that k = 2, λ = 0, ρ = 0, the class Pλ k (ρ) reduces to the class P of functions p(z) analytic in U with p(0) = 1 and whose real part is positive. we recall the well-known classes Rλk(ρ) = ¨ f (z) : f (z) ∈ A and z f ′(z) f (z) ∈ Pλk (ρ), 0≤ ρ < 1 « , Vλk (ρ) = ¨ f (z) : f (z) ∈ A and (z f ′(z))′ f ′(z) ∈ Pλk (ρ), 0≤ ρ < 1 « . These classes are introduced and studied in [7]. The purpose of this paper is to develop the mapping properties with respect to a new generalized integral operator. 2. Preliminary Results Prof. Breaz [3] has introduced the following integral operators on univalent function spaces: J(z) =    β z ∫ 0 � f ′1(t n) �γ1 · . . . · h f ′p(t n) iγp d t    1 β , (4) H(z) =    β z ∫ 0 tβ−1 � f ′1(t) �γ1 · . . . · h f ′p(t) iγp d t    1 β , (5) F(z) = z ∫ 0 � f1(t) t �γ1 · . . . · � fp(t) t �γp d t, (6) I. Dorca, D. Breaz / Eur. J. Pure Appl. Math, 6 (2013), 11-19 13 G(z) =     β z ∫ 0 � f1(t) t �γ1 · . . . · � fp(t) t �γp d t     1 β , (7) Fγ,β (z) =    β z ∫ 0 tβ−1 � f1(t) t � 1 γ1 · . . . · � fp(t) t � 1 γp d t    1 β , (8) and Gγ,p(z) =    [p(γ− 1) + 1] z ∫ 0 g γ−1 1 (t) · . . . · gγ−1 p (t)d t    1 p(γ−1)+1 , (9) where γi,γ,β ∈ C∀i = 1, p, p ∈ N− {0}, n ∈ N− {0,1}. Let Dn be the Sălăgean differential operator [see 12] Dn :A →A , n ∈ N, defined as: D0 f (z) = f (z), D1 f (z) = D f (z) = z f ′(z), Dn f (z) = D(Dn−1 f (z)) (10) and Dk, Dk :A →A , k ∈ N∪ {0}, of form: D0 f (z) = f (z), . . . , Dk f (z) = D(Dk−1 f (z)) = z + ∞ ∑ n=2 nkanzn. (11) Definition 1 ([2]). Let β , λ ∈ R, β ≥ 0, λ ≥ 0 and f (z) = z + ∑∞ j=2 a jz j . We denote by D β λ the linear operator defined by D β λ : A→ A, D β λ f (z) = z + ∞ ∑ j=n+1 [1+ ( j− 1)λ]βa jz j . (12) Remark 1. In [1] we have introduced the following operator concerning the functions of form (1): D β λ : A→ A, D β λ f (z) = z − ∞ ∑ j=n+1 [1+ ( j− 1)λ]βa jz j . (13) The neighborhoods concerning the class of functions defined using the operator (13) is studied in [5]. Remark 2. Let consider the following operator concerning the functions f ∈ S, S = { f ∈A : f is univalent in U}: D n,β λ1 ,λ2 f (z) = (h ∗ψ1 ∗ f )(z) = z ± ∑ k≥2 [1−λ1(k− 1))]β−1 [1−λ2(k− 1))]β · 1+ c k+ c · C(n, k) · ak · z k, (14) where C(n, k) = (n+1)k−1 (1)k−1 , (·)· is the Pochammer symbol; k ≥ 2, c ≥ 0. I. Dorca, D. Breaz / Eur. J. Pure Appl. Math, 6 (2013), 11-19 14 The following integral operator is studied in [4], where fi, i = 1 . . . n, n ∈ N, is considered to be of form (2): Definition 2. We define the general integral operator Ik,n,λ,µ :An→A by Ik,n,λ,µ( f1, . . . , fn) = F , (15) DkF(z) = z ∫ 0 � Dλ1 f1(t) t �µ1 · . . . · � Dλn fn(t) t �µn d t, where fi ∈A , i ∈ N− {0}, λ= (λ1, . . . ,λn) ∈ N n 0, µ = (µ1, . . . ,µn) ∈ N n, n ∈ N and k ∈ N0. Theorem 1. Let α, γ1, γ2, β ∈ C, Re α = a > 0 and D n,κ λ1 ,λ2 f j(z) ∈ A , λ1, λ2, κ ≥ 0, σ ∈ R, j = 1, p, p ∈ N, D n,κ λ1,λ2 f j(z n) of form (14). If � � � � � (D n,κ λ1,λ2 f j(z n))′′ (D n,κ λ1,λ2 f j(z n))′ � � � � � ≤ 1 n and � � � � � (D n,κ λ1,λ2 f j(z n))′ (D n,κ λ1,λ2 f j(z n)) � � � � � ≤ 1 n ∀z ∈ U , j = 1, p, p ∑ j=1 [|δ1 j | · (|2γ1− 1| − |σ|)+ |δ2 j | · (|2γ2− 1| − |σ|)] |σ · (2γ1− 1) · (2γ2 − 1) · ( p ∏ j=1 δ1 j · δ2 j )| ≤ 1, and |σ · (2γ1− 1) · (2γ2− 1) · ( p ∏ j=1 δ1 j ·δ 2 j )| ≤ n+ 2a 2 · � n+ 2a n � 1 n+2a , then ∀δ, δ1 j , δ2 j ∈ C, j = 1 . . . p, Re(β)≥ a, Re(βδ)≥ a, the function I1(z) =    β z ∫ 0 tβδ−1 · p ∏ j=1   ((D n,κ λ1,λ2 f j(t n)′)2γ1−1 tσ   δ1 j ·   (D n,κ λ1,λ2 f j(t n))2γ2−1 tσ   δ2 j d t    1 β (16) is univalent for all n ∈ N− {0}. If we consider the operator D β λ f (z) of form (13) we obtain the following Corollary, whose proof is similar with the prove of Theorem 1. Corollary 1. Let α, γ1, γ2, χ ∈ C, Re α = a > 0 and D β λ f j(z) ∈ A , β ≥ 0, λ ≥ 0, σ ∈ R, D β λ f (zn) of form (13). If � � � � � (D β λ f j(z n))′′ (D β λ f j(z n))′ � � � � � ≤ 1 n and � � � � � (D β λ f j(z n))′ (D β λ f j(z n)) � � � � � ≤ 1 n , ∀z ∈ U , j = 1, p, I. Dorca, D. Breaz / Eur. J. Pure Appl. Math, 6 (2013), 11-19 15 p ∑ j=1 [|δ1 j | · (|2γ1− 1| − |σ|)+ |δ2 j | · (|2γ2− 1| − |σ|)] |σ · (2γ1− 1) · (2γ2− 1) · ( p ∏ j=1 δ1 j ·δ2 j )| ≤ 1 and |σ · (2γ1− 1) · (2γ2− 1) · ( p ∏ j=1 δ1 j ·δ 2 j )| ≤ n+ 2a 2 · � n+ 2a n � 1 n+2a , then for all δ, δ1 j , δ 2 j ∈ C, j = 1 . . . p, Re(χ)≥ a, Re(χδ)≥ a, the function I2(z) =    χ z ∫ 0 tχδ−1 p ∏ j=1   ((D β λ f j(t n)′)2γ1−1 tσ   δ1 j   (D β λ f j(t n))2γ2−1 tσ   δ2 j d t    1 χ (17) is univalent for ∀n ∈ N− {0}. Lemma 1 ([6] ). Let u = u1 + iu2, v = v1 + iv2 and Ψ(u, v) be a complex valued function satisfying the conditions: (i) Ψ(u, v) is continuous in a domain D ∈ C2, Re (ii) (1,0) ∈ D and Re Ψ(1,0)> 0, (iii) Re Ψ(iu2, v1)≤ 0, whenever (iu2, v1) ∈ D and v1 ≤ − 1 2 (1+ u2 2). If h(z) = 1+ ∑ i≥1 ciz i is an analytic function in U such that (h(z), zh′(z)) ∈ D and Re Ψ(h(z), zh′(z))> 0 for z ∈ U , then Re h(z)> 0 in U . Lemma 2 ([8]). Let f (z) ∈ V λ k (ρ), 0 ≤ ρ < 1 and λ is real with |λ| < π 2 . Then f (z) ∈ Rλ k (β), where β is one of the root of 2β3 + (1− 2ρ)β2+ (3 sec2λ− 4)β − (1+ 2ρ) tan2λ= 0. (18) Following we present the mapping properties of the general integral operator of form (16), giving also several examples which prove its relevance. 3. Main Results Theorem 2. Let D n,κ λ1,λ2 f j(z n) ∈ Rλ k , D n,κ λ1,λ2 f j(z n) of form (14), n ∈ N, λ1, λ2, κ ≥ 0, σ ∈ R, j = 1, p p ∈ N, for 0≤ ρ < 1. Also let λ be real, |λ|< φ 2 . If 0≤ [ρ − 1] p ∑ j=1 δa j + βδ < 1, I. Dorca, D. Breaz / Eur. J. Pure Appl. Math, 6 (2013), 11-19 16 then I1(z) ∈ V λ k (η), I1(z) of form (16), with η = [ρ− 1] p ∑ j=1 δa j + βδ, (19) β , δ, δa j ∈ C, a ∈ {1,2}, j = 1, p, Re(βδ)> 0. Proof. Let consider the notations h(z) = z ∫ 0 tβδ−1 p ∏ j=1   ((D n,κ λ1,λ2 f j(t n)′)2γ1−1 tσ   δ1 j ·   (D n,κ λ1,λ2 f j(t n))2γ2−1 tσ   δ2 j d t = z ∫ 0 tβδ−1 p ∏ j=1 h h1 j (t n) iδ1 j · h h2 j (t n) iδ2 j d t in (16), with α, γ1, γ2, β , δ ∈ C, Re α = a > 0 and D n,κ λ1,λ2 f j(z) ∈ A , n ∈ N, λ1, λ2, κ ≥ 0, σ ∈ R, j = 1, p, p ∈ N. From Theorem 1, we obtain [I1(z)]′′ [I1(z)]′ = � 1 β − 1 � · h′(z) h(z) +βδ · 1 z +    p ∑ j=1,a∈{1,2} δa j · [ha j (z)] ′ ha j (z) − 1 z    which is equivalently to eiλ � 1+ z[I1(z)]′′ [I1(z)]′ � = eiλ· � � 1 β − 1 � · zh′(z) h(z) + βδ � +eiλ·    p ∑ j=1,a∈{1,2} δa j · z[ha j (z)]′ ha j (z) − 1   +eiλ (20) Furthermore, we have Re � eiλ � 1+ z[I1(z)]′′ [I1(z)]′ �� ≤ (βδ− 1)+ Re   e iλ ·    p ∑ j=1,a∈{1,2} δa j · z[ha j (z)]′ ha j (z) − 1   + eiλ    , which can be written as following Re � eiλ � 1+ z[I1(z)]′′ [I1(z)]′ �� ≤ Re   e iλ ·    p ∑ j=1,a∈{1,2} δa j · z[ha j (z)]′ ha j (z) − 1   + βδeiλ    . Subtracting and adding ρ cosλ p ∑ j=1,a∈{1,2} δa j on the left hand side of (20) and then taking the real part, we have Re � eiλ � 1+ z[I1(z)]′′ [I1(z)]′ � −η cosλ � ≤ p ∑ j=1,a∈{1,2} δa j Re  eiλ · [ha j (z)] ′ ha j (z) −ρ cosλ   , (21) I. Dorca, D. Breaz / Eur. J. Pure Appl. Math, 6 (2013), 11-19 17 where η is given by (19). Integrating (21) and then using (19), we have ∫ 2π 0 � � � � � Re � eiλ � 1+ z[I1(z)]′′ [I1(z)]′ � −η cosλ � � � � � � dθ ≤ 1−η 1−ρ ∫ 2π 0 � � � � � Re  eiλ · [ha j (z)]′ ha j (z) −ρ cosλ   � � � � � dθ . (22) Since f j(z n) ∈ Rλ k (ρ), j = 1, p, p, n ∈ N− {0}, we obtain ∫ 2π 0 � � � � � Re  eiλ · [ha j (z)]′ ha j (z) −ρ cosλ   � � � � � dθ ≤ (1−ρ)kπ cosλ. (23) Using (22) and (23), we have ∫ 2π 0 � � � � � Re � eiλ � 1+ z[I1(z)]′′ [I1(z)]′ � −η cosλ � � � � � � dθ ≤ (1−η)kπ cosλ. Hence I1(z) ∈ V λ k (η) with η given by (19). Remark 3. If we consider the operator D β λ f (z) ∈ Rλ k (ρ) of form (13) we obtain similar result as in Theorem 2. Remark 4. If we apply the operator (10) to the integral operator F(z) of form (6), we obtain the result from [8]. Next we give few examples of particular cases which can be found in literature. Let β = 0 in D β λ f (z) of form (12) or (13). So we have that D0 λ f (z) = f (z),∀λ ≥ 0. We will use this form of the integral operator, where the function f is of form (2) with respect to the operator (17). For further simplification, we consider that γ1 = γ2 = 1, and δ = 1 (except of Example 4). For the first four examples we consider δ1 j = 0, j = 1, p, p ∈ N−{0}, n= 1. Example 1. If σ = 1, χ = 1 and we use the notation δ2 j = γ j, j = 1, p, p ∈ N−{0}, we obtain the operator F(z) of form (6). F(z) ∈ V λ k (η) if 0≤ (ρ−1) p ∑ j=1 γ j+1< 1 with η = (ρ−1) p ∑ j=1 γ j+1. Example 2. If σ = 1 we obtain the operator G(z) of form (7) for δ2 j = γ j , j = 1, p, p ∈ N−{0}. G(z) ∈ V λ k (η) if 0≤ (ρ− 1) p ∑ j=1 γ j + 1< 1 with η= (ρ− 1) p ∑ j=1 γ j + 1. REFERENCES 18 Example 3. If σ = 1 and we use the notation δ2 j = 1/γ j, j = 1, p, p ∈ N− {0}, we obtain the operator Fγ,β (z) of form (8). Fγ,β(z) ∈ Vλ k (η) if 0≤ (ρ− 1) p ∑ j=1 1 γ j + β < 1 with η = (ρ− 1) p ∑ j=1 γ j + β . Example 4. If σ = 0 we obtain the operator Gγ,p(z) of form (9) for χ = [p(γ− 1) + 1], δ = 1 χ and δ2 j = γ− 1, Gγ,p(z) ∈ Vλ k (η) if 0≤ (1−ρ) p ∑ j=1 γ j + 1< 1 with η = (ρ− 1) p ∑ j=1 γ j + 1. For the next two examples we consider δ2 j = 0, j = 1, p, p ∈ N− {0}, and σ = 0. Example 5. a) If χ = 1, δ = 1, we obtain a particular case of the function J(z) of form (4), in which β = 1,∀n ∈ N − {0}. J(z) ∈ Vλ k (η) if 0 ≤ (1− ρ) p ∑ j=1 γ j + 1 < 1 with η = (ρ− 1) p ∑ j=1 γ j + 1. b) If δ = 1 χ , δ1 j = γ j , j = 1, p, p ∈ N−{0}, we obtain the operator J(z) of form (4), in which β = 1,∀n ∈ N−{0}. J(z) ∈ Vλ k (η) if 0≤ (1−ρ) p ∑ j=1 γ j+1< 1 with η = (ρ−1) p ∑ j=1 γ j+1. Example 6. If n = 1, δ = 1 χ , we obtain the operator H(z) of form (5) for δ1 j = γ j , j = 1, p, p ∈ N− {0}. F(z) ∈ V λ k (η) if 0≤ (1−ρ) p ∑ j=1 γ j + β < 1 with η = (ρ− 1) p ∑ j=1 γ j + β . ACKNOWLEDGEMENTS This work was partially supported by the strategic project POSDRU 107/1.5/S/77265, inside POSDRU Romania 2007-2013 co-financed by the European Social Fund-Investing in People. The authors thank the readers of European Journal of Pure and Applied Mathematics, for making our journal successful. References [1] M. Acu, I. Dorca, and S. Owa. On some starlike functions with negative coefficients. In Daniel v. Breaz, editor, Proceedings of the Interational Coference on Theory and Applica- tions of Mathematics and Informatics., pages 101–112, Alba Iulia, 2011. ICTAMI. [2] M. Acu and S. Owa. Note on a class of starlike functions. In Proceeding Of the Inter- national Short Joint Work on Study on Calculus Operators in Univalent Function Theory., pages 1–10, Kyoto, 2006. [3] D. Breaz. Integral operators on univalent function spaces. Editura Academiei Române., Bucureşti, 2004. REFERENCES 19 [4] D. Breaz, H. O. Güney, and G. Ş. Sălăgean. A new general integral operator. 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