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Bernardi-Libera-Livingston Integral Operator M. Eshaghi Gordji, D. Alimohammadi and A. Ebadian

vol. 10, iss. 4, art. 100, 2009

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SOME APPLICATIONS OF THE GENERALIZED BERNARDI–LIBERA–LIVINGSTON INTEGRAL

OPERATOR ON UNIVALENT FUNCTIONS

M. ESHAGHI GORDJI D. ALIMOHAMMADI

Dept, of Mathematics, Faculty of Science Department of Mathematics Semnan University, Semnan, Iran Arak University, Arak, Iran

EMail:madjideshaghi@gmail.com EMail:d-alimohammadi@araku.ac.ir

A. EBADIAN

Dept. of Mathematics, Faculty of Science Urmia University, Urmia, Iran

EMail:ebadian.ali@gmail.com Received: 17 October, 2008

Accepted: 24 July, 2009

Communicated by: S.S. Dragomir 2000 AMS Sub. Class.: 30C45, 30C50.

Key words: Analytic function, Integral operator, Univalent function.

Abstract: In this paper by making use of the generalized Bernardi–Libera–Livingston inte- gral operator we introduce and study some new subclasses of univalent functions.

Also we investigate the relations between those classes and the classes which are studied by Jin–Lin Liu.

Acknowledgements: The authors would like to thank the referee for a number of valuable suggestions regarding of a previous version of this paper.

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Bernardi-Libera-Livingston Integral Operator M. Eshaghi Gordji, D. Alimohammadi and A. Ebadian

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Contents

1 Introduction 3

2 Main Results 7

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1. Introduction

LetAbe the class of functions of the form,f(z) = z+P

n=2anznwhich are analytic in the unit diskU ={z :|z|<1}. Also, letSdenote the subclass ofAconsisting of all univalent functions inU. Supposeλis a real number with0≤λ <1. A function f ∈ S is said to be starlike of order λ if and only if Renzf0(z)

f(z)

o

> λ, z ∈ U. Also, f ∈ S is said to be convex of order λ if and only ifRen

1 + zff000(z)(z)

o

> λ, z ∈ U. We denote by S(λ), C(λ)the classes of starlike and convex functions of order λ respectively. It is well known that f ∈ C(λ) if and only if zf0∗(λ). If f ∈ A,thenf ∈K(β, λ)if and only if there exists a functiong ∈ S(λ)such that Re

nzf0(z) g(z)

o

> β, z ∈ U, where0 ≤ β < 1. These functions are called close-to- convex functions of order β type λ. A function f ∈ A is called quasi-convex of orderβ typeλif there exists a functiong ∈ C(λ)such thatRen

(zf0(z))0 g0(z)

o

> β. We denote this class byK(β, λ)[10]. It is easy to see thatf ∈K(β, γ)if and only if zf0 ∈K(β, γ)[9]. Forf ∈Aif for someλ(0≤λ <1)andη(0< η ≤1)we have (1.1)

arg

zf0(z) f(z) −λ

< π

2η, (z ∈U),

thenf(z)is said to be strongly starlike of orderηand typeλinU and we denote this class byS(η, λ). Iff ∈Asatisfies the condition

(1.2)

arg

1 + zf00(z) f0(z) −λ

< π

2η, (z ∈U)

for someλandηas above, then we say thatf(z)is strongly convex of orderη and typeλinU and we denote this class byC(η, λ). Clearlyf ∈ C(η, λ)if and only if zf0∗(η, λ), and in particular, we haveS(1, λ) = S(λ)andC(1, λ) = C(λ).

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Bernardi-Libera-Livingston Integral Operator M. Eshaghi Gordji, D. Alimohammadi and A. Ebadian

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For c > −1 and f ∈ A the generalized Bernardi–Libera–Livingston integral operatorLcf is defined as follows

(1.3) Lcf(z) = c+ 1

zc Z z

0

tc−1f(t)dt.

This operator forc∈ N = {1,2,3, . . .}was studied by Bernardi [1] and forc = 1 by Libera [4] (see also [8]). The classesSTc(η, λ)and CVc(η, λ) were introduced by Liu [7], where

STc(η, λ) =

f ∈A:Lcf ∈S(η, λ),z(Lcf(z))0

Lcf(z) 6=λ, z ∈U

, CVc(η, λ) =

f ∈A:Lcf ∈C(η, λ),(z(Lcf(z))0)0

(Lcf(z))0 6=λ, z ∈U

.

Now by making use of the operator given by (1.3) we introduce the following classes.

Sc(λ) ={f ∈A:Lcf ∈S(λ)}, Cc(λ) ={f ∈A:Lcf ∈C(λ)}.

Obviously f ∈ CVc(η, λ) if and only if zf0 ∈ STc(η, λ). J. L. Liu [5] and [6]

introduced and similarly investigated the classesSσ(λ), Cσ(λ),Kσ(β, λ),Kσ(β, λ), STσ(η, λ), CVσ(η, λ)by making use of the integral operatorIσf given by

(1.4) Iσf(z) = 2σ zΓ(σ)

Z z

0

log z

t σ−1

f(t)dt, σ >0, f ∈A.

The operator Iσ was introduced by Jung, Kim and Srivastava [2] and then investi- gated by Uralegaddi and Somanatha [13], Li [3] and Liu [5]. For the integral opera-

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Bernardi-Libera-Livingston Integral Operator M. Eshaghi Gordji, D. Alimohammadi and A. Ebadian

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tors given by(1.3)and(1.4)we have verified following relationships.

(1.5) Iσf(z) = z+

X

n=2

2 n+ 1

σ

anzn,

(1.6) Lcf(z) =z+

X

n=2

c+ 1 n+canzn, (1.7) z(IσLcf(z))f(z)−cIσLcf(z),

(1.8) z(LcIσf(z))f(z)−cLcIσf(z).

It follows from(1.5)that one can define the operatorIσfor any real numberσ. In this paper we investigate the properties of the classesSc(λ), Cc(λ), Kc(β, λ), Kc(β, λ), STc(η, λ) andCVc(η, λ). We also study the relations between these classes by the classes which are introduced by Liu in [5] and [6]. For our purposes we need the following lemmas.

Lemma 1.1 ([9]). Let u = u1 +iu2, v = v1 +iv2 and let ψ(u, v) be a complex functionψ :D⊂C×C→C. Suppose thatψ satisfies the following conditions

(i) ψ(u, v)is continuous inD;

(ii) (1,0)∈DandRe{ψ(1,0)}>0;

(iii) Re{ψ(iu2, v1)} ≤0for all(iu2, v1)∈Dwithv1 ≤ −1+u2 22. Letp(z) = 1 +P

n=2cnznbe analytic inU so that(p(z), zp0(z)) ∈ Dfor all z ∈U. IfRe{ψ(p(z), zp0(z))}>0, z∈U thenRe{p(z)}>0, z ∈U.

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Lemma 1.2 ([11]). Let the function p(z) = 1 + P

n=1cnzn be analytic inU and p(z) 6= 0, z ∈ U. If there exists a point z0 ∈ U such that|arg(p(z))| < π2η for

|z| < |z0| and argp(z0)| = π2η where 0 < η ≤ 1, then z0p(zp0(z0)

0) = ikη and k ≥

1

2(r+ 1r)when argp(z0) = π2η,Also, k ≤ −12 (r+ 1r)whenargp(z0) = −π2 η, and p(z0)1/η =±ir(r >0).

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Bernardi-Libera-Livingston Integral Operator M. Eshaghi Gordji, D. Alimohammadi and A. Ebadian

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2. Main Results

In this section we obtain some inclusion theorems by following the method of proof adopted in [12].

Theorem 2.1.

(i) Forf ∈ Aif Ren

zf0(z)

f(z)z(LLcf(z))0

cf(z)

o

> 0and z(LLc+1f(z))0

c+1f(z) is an analytic func- tion, thenSc(λ)⊂Sc+1 (λ).

(ii) Letc > −λ. For f ∈ AifRen

zf0(z)

f(z)z(LLc+1f(z))0

c+1f(z)

o

>0and z(LLc+1f(z))0

c+1f(z) is an analytic function, thenSc+1 (λ)⊂Sc(λ).

Proof. (i) Suppose thatf ∈Sc(λ)and set

(2.1) z(Lc+1f(z))0

Lc+1f(z) −λ= (1−λ)p(z), wherep(z) = 1 +P

n=2cnzn. An easy calculation shows that (2.2)

z(Lc+1f(z))0 Lc+1f(z)

h

2 +c+z(L(Lc+1f(z))00

c+1f(z))0

i

z(Lc+1f(z))0

Lc+1f(z) +c+ 1 = zf0(z) f(z) . By settingH(z) = z(LLc+1f(z))0

c+1f(z) we have (2.3) 1 + z(Lc+1f(z))00

(Lc+1f(z))0 =H(z) + zH0(z) H(z) .

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By making use of(2.3)in(2.2),sinceH(z) =λ+ (1−λ)p(z), we obtain (2.4) (1−λ)p(z) + (1−λ)zp0(z)

λ+c+ 1 + (1−λ)p(z) = zf0(z) f(z) −λ.

If we consider

ψ(u, v) = (1−λ)u+ (1−λ)v

λ+c+ 1 + (1−λ)u, then ψ(u, v) is a continuous function in D =

C−λ+c+1λ−1 ×C and(1,0) ∈ D.

Also,ψ(1,0)>0and for all(iu2, v1)∈Dwithv1 ≤ −1+u2 22 we have Reψ(iu2, v1) = (1−λ)(λ+c+ 1)v1

(1−λ)2u22+ (λ+c+ 1)2

≤ −(1−λ)(λ+c+ 1)(1 +u22) 2[(1−λ)2u22+ (λ+c+ 1)2] <0.

Therefore the function ψ(u, v) satisfies the conditions of Lemma 1.1 and since in view of the assumption, by considering (2.4),we have Re{ψ(p(z), zp0(z))} > 0, Lemma1.1implies thatRep(z)>0, z ∈U and this completes the proof of (i).

(ii) For proving this part of the theorem, we use the same method and a easily verified formula similar to (2.2). By replacing c+ 1 with c we get the desired result.

Theorem 2.2.

(i) Forf ∈ Aif Ren

zf0(z)

f(z)z(LLcf(z))0

cf(z)

o

> 0and z(LLc+1f(z))0

c+1f(z) is an analytic func- tion, thenCc(λ)⊂Cc+1(λ).

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Bernardi-Libera-Livingston Integral Operator M. Eshaghi Gordji, D. Alimohammadi and A. Ebadian

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(ii) Letc > −λ. For f ∈ AifRen

zf0(z)

f(z)z(LLc+1f(z))0

c+1f(z)

o

>0and z(LLc+1f(z))0

c+1f(z) is an analytic function, thenCc+1(λ)⊂Cc(λ).

Proof. (i) In view of part (i) of Theorem2.1we can write

f ∈Cc(λ)⇔Lcf ∈C(λ)⇔z(Lcf)0∗(λ)⇔Lczf0∗(λ)⇔zfc0∗(λ)⇒zfc+10∗ (λ)

⇔Lc+1zf0∗(λ)⇔z(Lc+1f)0∗(λ)⇔Lc+1f ∈C(λ)⇔f ∈Cc+1(λ).

Part (ii) of the theorem can be proved in a similar manner.

Theorem 2.3. Ifc≥ −λ and zff(z)0(z) is an analytic function, thenf ∈ S(λ)implies f ∈Sc(λ).

Proof. By differentiating logarithmically both sides of (1.3) with respect to z we obtain

(2.5) z(Lcf(z))0

Lcf(z) +c= (c+ 1)f(z) Lcf(z) . Again differentiating logarithmically both sides of(2.5)we have

(2.6) p(z) + zp0(z)

c+λ+p(z) = zf0(z) f(z) −λ, where p(z) = z(LLcf(z))0

cf(z) −λ. Let us consider ψ(u, v) = u+ u+c+λv . Then ψ is a continuous function inD={C−(−c−λ)} ×C,(1,0)∈D andRe ψ(1,0)>0.

If(iu2, v1)∈Dwithv1 ≤ −1+u2 22,then

Reψ(iu2, v1) = v1(c+λ)

u22+ (c+λ)2 ≤0.

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Sincef ∈S(λ),then(2.6)gives

Re(ψ(p(z), zp0(z))) = Re

zf0(z) f(z) −λ

>0.

Therefore Lemma 1.1 concludes that Re{p(z)} > 0 and this completes the proof.

Corollary 2.4. Ifc ≥ λand zff(z)0(z) is an analytic function, then f ∈ C(λ)implies f ∈Cc(λ).

Proof. We have

f ∈C(λ)⇔zf0∗(λ)Λzfc0∗(λ)⇔Lczf0 ∈S(λ)

⇔z(Lcf)0∗(λ)⇔Lcf ∈C(λ)⇔f ∈Cc(λ).

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References

[1] S.D. BERNARDI, Convex and starlike univalent functions, Trans. Amer. Math.

Soc., 135 (1969), 429–446.

[2] I.B. JUNG, Y.C. KIMANDH.M. SRIVASTAVA, The Hardy space of analytic functions associated with certain one-parameter families of integral operators, J. Math. Anal. Appl., 176 (1993), 138–147.

[3] J.L. LI, Some properties of two integral operators, Soochow. J. Math., 25 (1999), 91–96.

[4] R.J. LIBERA, Some classes of regular functions, Proc. Amer. Math. Soc.,16 (1965), 755–758.

[5] J.L. LIU, A linear operator and strongly starlike functions, J. Math. Soc. Japan, 54(4) (2002), 975–981.

[6] J.L. LIU, Some applications of certain integral operator, Kyungpook Math. J., 43(2003), 21–219.

[7] J.L. LIU, Certain integral operator and strongly starlike functions, Int. J. Math.

Math. Sci., 30(9) (2002), 569–574.

[8] A.E. LIVINGSTON, On the radius of univalence of certain analytic functions, Proc. Amer. Math. Soc., 17 (1996), 352–357.

[9] S.S. MILLER and P.T. MOCANU, Second order differential inequalities in the complex plane, J. Math. Anal. Appl., 65 (1978), 289–305.

[10] K.I. NOOR, On quasi-convex functions and related topics, Internat. J. Math.

Math. Sci.,10 (1987), 241–258.

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[11] M. NUNOKAWA, S. OWA, H. SAITOH, A. IKEDA AND N. KOIKE, Some results for strongly starlike functions, J. Math. Anal. Appl., 212 (1997), 98–

106.

[12] J. SOKOL, A linear operator and associated class of multivalent analytic func- tions, Demonstratio Math., 40(3) (2007), 559–566.

[13] B.A. URALEGADDI AND C. SOMANATHA, Certain integral operators for starlike functions, J. Math. Res. Expo., 15 (1995), 14–16.

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