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12. An Application of Hypergeometric Functions on Harmonic Univalent Functions

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ISSN: 1821-1291, URL: http://www.bmathaa.org Volume 2 Issue 4(2010), Pages 97-105.

AN APPLICATION OF HYPERGEOMETRIC FUNCTIONS ON HARMONIC UNIVALENT FUNCTIONS

(DEDICATED IN OCCASION OF THE 70-YEARS OF PROFESSOR HARI M. SRIVASTAVA)

SAURABH PORWAL AND KAUSHAL KISHORE DIXIT

Abstract. The purpose of the present paper is to establish connections

be-tween various subclasses of harmonic functions by applying certain convolu-tion operator involving hypergeometric funcconvolu-tions. To be more precise, we investigate such connections with Goodman-Rønning-type harmonic univalent functions in the open unit disc𝑈.

1. Introduction

Let𝐴denote the class of functions of the form

𝑓(𝑧) =𝑧+

𝑛=2

𝑎𝑛𝑧𝑛 (1.1)

which are analytic in the open unit disc𝑈. Hohlov [8] introduced the convolution operator𝐻(𝑎, 𝑏;𝑐) :𝐴→𝐴defined by

𝐻(𝑎, 𝑏;𝑐)𝑓(𝑧) =𝑧𝐹(𝑎, 𝑏;𝑐;𝑧)∗𝑓(𝑧),

where the symbol ”∗” stands for the convolution of two power series, which is defined

for two functions𝑓, 𝑔∈𝐴, where𝑓(𝑧) and𝑔(𝑧) are of the form𝑓(𝑧) =𝑧+

𝑛=2 𝑎𝑛𝑧𝑛

and𝑔(𝑧) =𝑧+

𝑛=2

𝑏𝑛𝑧𝑛 as

2000Mathematics Subject Classification. 30C45, 30C50, 33A30.

Key words and phrases. Harmonic, Starlike, Convex, Hypergeometric functions. c

⃝2008 Universiteti i Prishtin¨es, Prishtin¨e, Kosov¨e.

The authors are thankful to the referee for his valuable comments and suggestions.

The present investigation was supported by the University grant commission under grant No. F. 11-12/2006(SA-I).

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(𝑓∗𝑔)(𝑧) =𝑓(𝑧)∗𝑔(𝑧) =𝑧+

𝑛=2

𝑎𝑛𝑏𝑛𝑧𝑛and𝐹(𝑎, 𝑏;𝑐;𝑧) is a well-known Gaussian

hypergeometric function and given by the series

𝐹(𝑎, 𝑏;𝑐;𝑧) =

𝑛=0

(𝑎)𝑛(𝑏)𝑛

(𝑐)𝑛(1)𝑛

𝑧𝑛,

where 𝑎, 𝑏, 𝑐 are complex numbers such that 𝑐 ∕= 0,−1,−2, ... and (𝑎)𝑛 is the

Pochhammer symbol defined in terms of the Gamma function, by

(𝑎)𝑛=

Γ(𝑎+𝑛) Γ(𝑎)

= {

1 if𝑛= 0

𝑎(𝑎+ 1)...(𝑎+𝑛−1) if𝑛∈𝑁 ={1,2,3...}.

A hypergeometric function𝐹(𝑎, 𝑏;𝑐;𝑧) is analytic in𝑈 and plays an important role in Geometric Function Theory. See, for example, the works by Ahuja [3], Carleson and Shaffer [5], Miller and Mocanu [9], Owa and Srivastava [10], Ponnusamy and Rønning [11], Ruscheweyh and Singh [13] and Swaminathan [14].

Let𝐻 be the family of all harmonic functions of the form𝑓 =ℎ+𝑔, where

ℎ(𝑧) =𝑧+

𝑛=2

𝐴𝑛𝑧𝑛, 𝑔(𝑧) = ∞

𝑛=1

𝐵𝑛𝑧𝑛, ∣𝐵1∣<1, (𝑧∈𝑈), (1.2)

are in the class𝐴. For complex parameters𝑎1, 𝑏1, 𝑐1, 𝑎2, 𝑏2, 𝑐2(𝑐1, 𝑐2∕= 0,−1,−2, ...), we define the functions Φ1(𝑧) =𝑧𝐹(𝑎1, 𝑏1;𝑐1;𝑧) and Φ2(𝑧) =𝑧𝐹(𝑎2, 𝑏2;𝑐2;𝑧) .

Corresponding to these functions, we consider the following convolution operator

Ω≡Ω (

𝑎1, 𝑏1, 𝑐1 𝑎2, 𝑏2, 𝑐2 )

:𝐻→𝐻

defined by

Ω (

𝑎1, 𝑏1, 𝑐1 𝑎2, 𝑏2, 𝑐2 )

𝑓 =𝑓∗(Φ1+ Φ2) =ℎ∗Φ1+𝑔∗𝜙2

for any function𝑓 =ℎ+𝑔 in𝐻. Letting

Ω (

𝑎1, 𝑏1, 𝑐1 𝑎2, 𝑏2, 𝑐2 )

𝐹(𝑧) =𝐻(𝑧) +𝐺(𝑧),

we have

𝐻(𝑧) =𝑧+

𝑛=2

(𝑎1)𝑛−1(𝑏1)𝑛−1 (𝑐1)𝑛−1(1)𝑛−1

𝐴𝑛𝑧𝑛, 𝐺(𝑧) = ∞

𝑛=1

(𝑎2)𝑛−1(𝑏2)𝑛−1 (𝑐2)𝑛−1(1)𝑛−1

𝐵𝑛𝑧𝑛. (1.3)

We observe that

Ω (

𝑎1, 1, 𝑎1 𝑎2, 1, 𝑎2 )

𝑓(𝑧) =𝑓(𝑧) =𝑓(𝑧)∗ (

𝑧 1−𝑧 +

𝑧 1−𝑧

)

is the identity mapping.

This convolution operator Ω were defined and studied by the author in [2]. Denote by𝑆𝐻 the subclass of 𝐻 that are univalent and sense-preserving in 𝑈.

Note that 1𝑓−∣−𝐵1𝑓𝐵12 ∈𝑆𝐻 whenever𝑓 ∈𝑆𝐻. We also let the subclass𝑆𝐻0 of 𝑆𝐻

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The classes 𝑆𝐻0 and 𝑆𝐻 were first studied in [6]. Also, we let 𝐾𝐻0, 𝑆 ∗,0

𝐻 and 𝐶

0

𝐻

denote the subclasses of𝑆𝐻0 of harmonic functions which are, respectively, convex, starlike and close-to-convex in 𝑈. For definitions and properties of these classes, one may refer to ([1], [6]) or [7].

For 0≤𝛾 <1, let

𝑁𝐻(𝛾) = {

𝑓 ∈𝐻 : Re𝑓

(𝑧)

𝑧′ ≥𝛾, 𝑧=𝑟𝑒 𝑖𝜃𝑈

} ,

𝐺𝐻(𝛾) = {

𝑓 ∈𝐻: Re {

(

1 +𝑒𝑖𝛼)𝑧𝑓

(𝑧)

𝑓(𝑧) −𝑒

𝑖𝛼 }

≥𝛾, 𝛼∈𝑅, 𝑧∈𝑈 }

,

where

𝑧′= ∂ ∂𝜃

(

𝑧=𝑟𝑒𝑖𝜃)

, 𝑓′(𝑧) = ∂ ∂𝜃𝑓

( 𝑟𝑒𝑖𝜃)

.

Define

𝑇 𝑁𝐻(𝛾) =𝑁𝐻(𝛾)∩𝑇 and𝑇 𝐺𝐻(𝛾) =𝐺𝐻(𝛾)∩𝑇,

where𝑇 consists of the functions𝑓 =ℎ+𝑔 in𝑆𝐻 so thatℎand𝑔 are of the form

ℎ(𝑧) =𝑧−

𝑛=2

∣𝐴𝑛∣𝑧𝑛, 𝑔(𝑧) = ∞

𝑛=1

∣𝐵𝑛∣𝑧𝑛. (1.4)

The classes𝑁𝐻(𝛾) and 𝐺𝐻(𝛾) were initially introduced and studied, respectively,

in ([4], [12]). A function in 𝐺𝐻(𝛾) is called Goodman-Rønning-type harmonic

univalent function in𝑈.

Throughout this paper, we will frequently use the notations

Ω (𝑓) = Ω (

𝑎1, 𝑏1, 𝑐1 𝑎2, 𝑏2, 𝑐2

) 𝑓,

𝐷𝑛−1=

(∣𝑎1∣)𝑛1(∣𝑏1∣)𝑛1

(𝑐1)𝑛1(1)𝑛1 , 𝐸𝑛−1=

(∣𝑎2∣)𝑛1(∣𝑏2∣)𝑛1 (𝑐2)𝑛1(1)𝑛1 ,

and a well-known formula

𝐹(𝑎, 𝑏;𝑐; 1) =Γ (𝑐−𝑎−𝑏) Γ (𝑐)

Γ (𝑐−𝑎) Γ (𝑐−𝑏), Re (𝑐−𝑎−𝑏)>0.

The main object of this paper is to establish some important connections between the classes𝐾0

𝐻,𝑆 ∗,0

𝐻 ,𝐶𝐻0,𝑁𝐻(𝛾) and𝐺𝐻(𝛾) by applying the convolution operator

Ω.

2. Connections with Goodman-Rønning-type Harmonic Univalent

Functions

In order to establish connections between harmonic convex functions, we need following results in Lemma 2.1 [6], Lemma 2.2 [12] and Lemma 2.3 [2].

Lemma 2.1. If 𝑓 =ℎ+𝑔∈𝐾𝐻0 whereℎand𝑔 are given by (1.2), then

∣𝐴𝑛∣ ≤

𝑛+ 1

2 , ∣𝐵𝑛∣ ≤ 𝑛−1

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Lemma 2.2. Let 𝑓 =ℎ+𝑔 be given by (1.2). If

𝑛=2

(2𝑛−1−𝛾)∣𝐴𝑛∣+ ∞

𝑛=1

(2𝑛+ 1 +𝛾)∣𝐵𝑛∣ ≤1−𝛾, (2.1)

then 𝑓 is sense-preserving, Goodman-Rønning-type harmonic univalent functions in𝑈 and𝑓 ∈𝐺𝐻(𝛾).

Remark 1. In [12], it is also shown that 𝑓 = ℎ+𝑔 given by (1.4) is in the family 𝑇 𝐺𝐻(𝛾), if and only if the coefficient condition (2.1) holds. Moreover, if

𝑓 ∈𝑇 𝐺𝐻(𝛾), then

∣𝐴𝑛∣ ≤

1−𝛾

2𝑛−1−𝛾, 𝑛≥2,

∣𝐵𝑛∣ ≤

1−𝛾

2𝑛+ 1 +𝛾, 𝑛≥1.

Lemma 2.3. If 𝑎, 𝑏, 𝑐 >0, then

(𝑖)

𝑛=2

(𝑛−1)(𝑎)𝑛−1(𝑏)𝑛−1 (𝑐)𝑛1(1)𝑛1 =

𝑎𝑏

𝑐−𝑎−𝑏−1𝐹(𝑎, 𝑏;𝑐; 1), 𝑖𝑓 𝑐 > 𝑎+𝑏+ 1.

(𝑖𝑖)

𝑛=2

(𝑛−1)2(𝑎)𝑛−1(𝑏)𝑛−1 (𝑐)𝑛1(1)𝑛1 =

[ (𝑎) 2(𝑏)2 (𝑐−𝑎−𝑏−2)2+

𝑎𝑏 𝑐−𝑎−𝑏−1

]

𝐹(𝑎, 𝑏;𝑐; 1), 𝑖𝑓 𝑐 > 𝑎+𝑏+2.

(𝑖𝑖𝑖)

𝑛=2

(𝑛−1)3(𝑎)𝑛−1(𝑏)𝑛−1 (𝑐)𝑛1(1)𝑛1 =

[ (𝑎) 3(𝑏)3 (𝑐−𝑎−𝑏−3)3+

3 (𝑎)2(𝑏)2 (𝑐−𝑎−𝑏−2)2 +

𝑎𝑏 𝑐−𝑎−𝑏−1

]

𝐹(𝑎, 𝑏;𝑐; 1), 𝑖𝑓 𝑐 > 𝑎+𝑏+ 3.

Theorem 2.1. Let 𝑎𝑗, 𝑏𝑗 ∈𝐶∖ {0},𝑐𝑗 ∈𝑅 and𝑐𝑗 >∣𝑎𝑗∣+∣𝑏𝑗∣+ 2 for𝑗= 1,2. If

for some𝛾(0≤𝛾 <1), the inequality

𝑄1𝐹(∣𝑎1∣,∣𝑏1∣;𝑐1; 1) +𝑅1𝐹(∣𝑎2∣,∣𝑏2∣;𝑐2; 1)≤4 (1−𝛾)

is satisfied, then

Ω( 𝐾𝐻0)

⊂𝐺𝐻(𝛾),

where

𝑄1=

2 (∣𝑎1∣)2(∣𝑏1∣)2

(𝑐1− ∣𝑎1∣ − ∣𝑏1∣ −2)2 + (7−𝛾)

∣𝑎1𝑏1∣

(𝑐1− ∣𝑎1∣ − ∣𝑏1∣ −1) + 2 (1−𝛾),

𝑅1=

2 (∣𝑎2∣)2(∣𝑏2∣)2

(𝑐2− ∣𝑎2∣ − ∣𝑏2∣ −2)2 + (5 +𝛾)

∣𝑎2𝑏2∣

(𝑐2− ∣𝑎2∣ − ∣𝑏2∣ −1).

Proof. Let𝑓 =ℎ+𝑔∈𝐾0

𝐻 where ℎand𝑔 are of the form (1.2) with𝐵1= 0. We need to show that Ω (𝑓) = 𝐻+𝐺∈𝐺𝐻(𝛾), where𝐻 and𝐺 defined by (1.3) are

analytic functions in𝑈.

In view of Lemma 2.2, we need to prove that

𝑃1≤1−𝛾,

where

𝑃1=

𝑛=2

(2𝑛−1−𝛾)

(𝑎1)𝑛1(𝑏1)𝑛1

(𝑐1)𝑛1(1)𝑛1 𝐴𝑛 +

𝑛=2

(2𝑛+ 1 +𝛾)

(𝑎2)𝑛1(𝑏2)𝑛1

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In view of Lemma 2.1 and 2.3, it follows that

𝑃1≤ 1 2

𝑛=2

(𝑛+ 1) (2𝑛−1−𝛾)𝐷𝑛−1+ 1 2

𝑛=2

(𝑛−1) (2𝑛+ 1 +𝛾)𝐸𝑛−1

= 1 2

𝑛=2 [

2 (𝑛−1)2+ (5−𝛾) (𝑛−1) + 2 (1−𝛾)]𝐷𝑛−1+ 1 2

𝑛=2 [

2 (𝑛−1)2+ (3 +𝛾) (𝑛−1)]𝐸𝑛−1

=1

2𝑄1𝐹(∣𝑎1∣,∣𝑏1∣;𝑐1; 1) + 1

2𝑅1𝐹(∣𝑎2∣,∣𝑏2∣;𝑐2; 1)−(1−𝛾).

Now𝑃1≤1−𝛾 follows from the given condition.

Analogous to Theorem 2.1, we next find connections of the classes𝑆𝐻∗,0,𝐶𝐻0 with 𝐺𝐻(𝛾). However, we first need the following result which may be found in ([1], [6])

or [15].

Lemma 2.4. If𝑓 =ℎ+𝑔∈𝑆𝐻∗,0or𝐶𝐻0 withℎand𝑔as given by (1.2)with𝐵1= 0, then

∣𝐴𝑛∣ ≤

(2𝑛+ 1) (𝑛+ 1)

6 , ∣𝐵𝑛∣ ≤

(2𝑛−1) (𝑛−1)

6 .

Theorem 2.2. Let 𝑎𝑗, 𝑏𝑗 ∈𝐶∖ {0},𝑐𝑗 ∈𝑅 and𝑐𝑗 >∣𝑎𝑗∣+∣𝑏𝑗∣+ 3 for𝑗= 1,2. If

for some𝛾(0≤𝛾 <1), the inequality

𝑄2𝐹(∣𝑎1∣,∣𝑏1∣;𝑐1; 1) +𝑅2𝐹(∣𝑎2∣,∣𝑏2∣;𝑐2; 1)≤12 (1−𝛾)

is satisfied, then

Ω(𝑆𝐻∗,0)⊂𝐺𝐻(𝛾)andΩ(𝐶𝐻0 )

⊂𝐺𝐻(𝛾),

where

𝑄2= 4 (∣𝑎1∣)3(∣𝑏1∣)3 (𝑐1− ∣𝑎1∣ − ∣𝑏1∣ −3)3

+ 2 (14−𝛾) (∣𝑎1∣)2(∣𝑏1∣)2 (𝑐1− ∣𝑎1∣ − ∣𝑏1∣ −1)2

+ 3 (13−3𝛾) ∣𝑎1𝑏1∣ (𝑐1− ∣𝑎1∣ − ∣𝑏1∣ −1)

+ 6 (1−𝛾),

𝑅2= 4 (∣𝑎2∣)3(∣𝑏2∣)3

(𝑐2− ∣𝑎2∣ − ∣𝑏2∣ −3)3+2 (10 +𝛾)

(∣𝑎2∣)2(∣𝑏2∣)2

(𝑐2− ∣𝑎2∣ − ∣𝑏2∣ −1)2+3 (5 +𝛾)

∣𝑎2𝑏2∣

(𝑐2− ∣𝑎2∣ − ∣𝑏2∣ −1).

Proof. Let𝑓 =ℎ+𝑔∈𝑆∗𝐻,0(𝐶0

𝐻) whereℎand𝑔of the form (1.2) with𝐵1= 0. We

need to show that Ω (𝑓) = 𝐻+𝐺∈𝐺𝐻(𝛾), where𝐻 and𝐺 defined by (1.3) are

analytic functions in𝑈.

In view of Lemma 2.2, we need to prove that

𝑃1≤1−𝛾,

where

𝑃1=

𝑛=2

(2𝑛−1−𝛾)

(𝑎1)𝑛1(𝑏1)𝑛1

(𝑐1)𝑛1(1)𝑛1 𝐴𝑛 +

𝑛=2

(2𝑛+ 1 +𝛾)

(𝑎2)𝑛1(𝑏2)𝑛1

(𝑐2)𝑛1(1)𝑛1 𝐵𝑛 .

In view of Lemma 2.3 and 2.4, it follows that

𝑃1≤ 1 6

𝑛=2

[(2𝑛+ 1) (𝑛+ 1) (2𝑛−1−𝛾)]𝐷𝑛−1+ 1 6

𝑛=2

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= 1 6

𝑛=2 [

4 (𝑛−1)3+ 2 (8−𝛾) (𝑛−1)2+ (19−7𝛾) (𝑛−1) + 6 (1−𝛾)]𝐷𝑛−1

+1 6

𝑛=2 [

4 (𝑛−1)3+ 2 (4 +𝛾) (𝑛−1)2+ (3 +𝛾) (𝑛−1)]𝐸𝑛−1

=1

6𝑄2𝐹(∣𝑎1∣,∣𝑏1∣;𝑐1; 1) + 1

6𝑅2𝐹(∣𝑎2∣,∣𝑏2∣;𝑐2; 1)−(1−𝛾)

Now𝑃1≤1−𝛾 follows from the given condition.

In order to determine connection between 𝑇 𝑁𝐻(𝛽) and 𝐺𝐻(𝛾), we need the

following results in Lemma 2.5 [4] and Lemma 2.6 [3].

Lemma 2.5. Let 𝑓 = ℎ+𝑔 where ℎ and 𝑔 as given by (1.4) with 𝐵1 = 0, and suppose that0≤𝛽 <1. Then

𝑓 ∈𝑇 𝑁𝐻(𝛽)⇔ ∞

𝑛=2

𝑛∣𝐴𝑛∣+ ∞

𝑛=2

𝑛∣𝐵𝑛∣ ≤1−𝛽.

Remark 2. If 𝑓 ∈𝑇 𝑁𝐻(𝛽), then

∣𝐴𝑛∣ ≤

1−𝛽

𝑛 , 𝑛≥2,

∣𝐵𝑛∣ ≤

1−𝛽

𝑛 , 𝑛≥1.

Lemma 2.6. Let 𝑎, 𝑏 ∈ 𝐶∖ {0}, 𝑎 ∕= 1, 𝑏 ∕= 1, 𝑐 ∈ (0,1)∪(1,∞) and 𝑐 > max{0,∣𝑎∣+∣𝑏∣ −1}. Then

𝑛=1 1 𝑛

(∣𝑎∣)𝑛1(∣𝑏∣)𝑛1 (𝑐)𝑛1(1)𝑛1 =

(𝑐− ∣𝑎∣ − ∣𝑏∣)

(∣𝑎∣ −1) (∣𝑏∣ −1)𝐹(∣𝑎∣,∣𝑏∣;𝑐; 1)−

(𝑐−1) (∣𝑎∣ −1) (∣𝑏∣ −1).

Theorem 2.3. Let𝑎𝑗, 𝑏𝑗 ∈𝐶∖ {0},𝑎𝑗∕= 1, 𝑏𝑗 ∕= 1,𝑐𝑗∈𝑅and𝑐𝑗>max{0,∣𝑎𝑗∣+∣𝑏𝑗∣ −1}

for𝑗= 1,2. If for some 𝛽(0≤𝛽 <1) and𝛾(0≤𝛾 <1), the inequality

𝑄3𝐹(∣𝑎1∣,∣𝑏1∣;𝑐1; 1) +𝑅3𝐹(∣𝑎2∣,∣𝑏2∣;𝑐2; 1)≤ (1−𝛾) (2−𝛽) (1−𝛽)

−(1 +𝛾)

[ (𝑐

1−1)

(∣𝑎1∣ −1) (∣𝑏1∣ −1)−

(𝑐2−1) (∣𝑎2∣ −1) (∣𝑏2∣ −1)

]

is satisfied, then

Ω (𝑇 𝑁𝐻(𝛽))⊂𝐺𝐻(𝛾),

where

𝑄3= 2−(1 +𝛾)

(𝑐1− ∣𝑎1∣ − ∣𝑏1∣) (∣𝑎1∣ −1) (∣𝑏1∣ −1)

and

𝑅3= 2 + (1 +𝛾)

(7)

Proof. Let 𝑓 = ℎ+𝑔 ∈ 𝑇 𝑁𝐻(𝛽) where ℎ and 𝑔 are given by (1.4). In view of

Lemma 2.2, it is enough to show that𝑃2≤1−𝛾, where

𝑃2=

𝑛=2

(2𝑛−1−𝛾)

(𝑎1)𝑛1(𝑏1)𝑛1

(𝑐1)𝑛1(1)𝑛1 𝐴𝑛 +

𝑛=1

(2𝑛+ 1 +𝛾)

(𝑎2)𝑛1(𝑏2)𝑛1

(𝑐2)𝑛1(1)𝑛1 𝐵𝑛 .

Using Remark 2 and Lemma 2.6, it follows that

𝑃2≤(1−𝛽) [

𝑛=2 (

2−(1 +𝛾) 𝑛

)

𝐷𝑛−1+

𝑛=1 (

2 + (1 +𝛾) 𝑛

) 𝐸𝑛−1

]

= (1−𝛽) [

𝑄3𝐹(∣𝑎1∣,∣𝑏1∣;𝑐1; 1) +𝑅3𝐹(∣𝑎2∣,∣𝑏2∣;𝑐2; 1)−(1−𝛾) + (1 +𝛾) (𝑐1−1) (∣𝑎1∣ −1) (∣𝑏1∣ −1) −

(1 +𝛾) (𝑐2−1) (∣𝑎2∣ −1) (∣𝑏2∣ −1)

]

≤1−𝛾,

by the given hypothesis.

In next theorem, we establish connections between𝑇 𝐺𝐻(𝛾) and𝐺𝐻(𝛾).

Theorem 2.4. Let 𝑎𝑗, 𝑏𝑗∈𝐶∖ {0},𝑐𝑗∈𝑅 and𝑐𝑗 >∣𝑎𝑗∣+∣𝑏𝑗∣ for𝑗= 1,2. If for

some𝛾(0≤𝛾 <1), the inequality

𝐹(∣𝑎1∣,∣𝑏1∣;𝑐1; 1) +𝐹(∣𝑎2∣,∣𝑏2∣;𝑐2; 1)≤2

is satisfied, then

Ω (𝑇 𝐺𝐻(𝛾))⊂𝐺𝐻(𝛾).

Proof. Making use of Lemma 2.2 and the definition of𝑃2 in Theorem 2.3, we only need to prove that𝑃2≤1−𝛾.

Using Remark 1, it follows that

𝑃2=

𝑛=2

(2𝑛−1−𝛾)

(𝑎1)𝑛1(𝑏1)𝑛1

(𝑐1)𝑛1(1)𝑛1 𝐴𝑛

+

𝑛=1

(2𝑛+ 1 +𝛾)

(𝑎2)𝑛1(𝑏2)𝑛1

(𝑐2)𝑛1(1)𝑛1 𝐵𝑛

≤(1−𝛾) [

𝑛=2

𝐷𝑛−1+

𝑛=1 𝐸𝑛−1

]

= (1−𝛾) [𝐹(∣𝑎1∣,∣𝑏1∣;𝑐1; 1)−1 +𝐹(∣𝑎2∣,∣𝑏2∣;𝑐2; 1)]

≤1−𝛾,

by the given condition and this completes the proof.

In the next result, we establish connections between 𝑇 𝐺𝐻(𝛾) and 𝐺𝐻(𝛾) by

diluting the restrictions on the complex coefficients of Theorem 2.4.

Theorem 2.5. If 𝑎1, 𝑏1 > −1, 𝑎1𝑏1 <0, 𝑐1 > max{0, 𝑎1+𝑏1}, 𝑎2, 𝑏2 ∈ 𝐶∖ {0} and𝑐2>∣𝑎2∣+∣𝑏2∣, then a sufficient condition for

Ω (𝑇 𝐺𝐻(𝛾))⊂𝐺𝐻(𝛾)

is that

𝐹(𝑎1, 𝑏1;𝑐1; 1)−𝐹(∣𝑎2∣,∣𝑏2∣;𝑐2; 1)≥0

(8)

Proof. Let𝑓 =ℎ+𝑔∈𝑇 𝐺𝐻(𝛾) withℎand𝑔 in (1.4). Then

Ω(𝑓) =𝑧−

𝑛=2

(𝑎1)𝑛1(𝑏1)𝑛1 (𝑐1)𝑛−1(1)𝑛−1

∣𝐴𝑛∣𝑧𝑛+ ∞

𝑛=1

(𝑎2)𝑛1(𝑏2)𝑛1 (𝑐2)𝑛−1(1)𝑛−1

∣𝐵𝑛∣𝑧𝑛.

This function can be rewritten as

Ω(𝑓) =𝑧+∣𝑎1𝑏1∣ 𝑐1

𝑛=2

(𝑎1+ 1)𝑛2(𝑏1+ 1)𝑛2

(𝑐1+ 1)𝑛2(1)𝑛1 ∣𝐴𝑛∣𝑧

𝑛

+

𝑛=1

(𝑎2)𝑛1(𝑏2)𝑛1

(𝑐2)𝑛1(1)𝑛1 ∣𝐵𝑛∣𝑧

𝑛.

In view of Lemma 2.2, we need to prove that𝑃3≤1−𝛾, where

𝑃3=

𝑛=2

(2𝑛−1−𝛾)∣𝑎1𝑏1∣ 𝑐1

(𝑎1+ 1)𝑛2(𝑏1+ 1)𝑛2

(𝑐1+ 1)𝑛2(1)𝑛1 𝐴𝑛

+

𝑛=1

(2𝑛+ 1 +𝛾)

(𝑎2)𝑛−1(𝑏2)𝑛−1

(𝑐2)𝑛1(1)𝑛1 𝐵𝑛

≤(1−𝛾) [

∣𝑎1𝑏1∣ 𝑎1𝑏1

𝑛=2

𝐷𝑛−1+

𝑛=1 𝐸𝑛−1

]

≤(1−𝛾) [−𝐹(𝑎1, 𝑏1;𝑐1; 1) + 1 +𝐹(∣𝑎2∣,∣𝑏2∣;𝑐2; 1)]

≤1−𝛾,

by the given condition.

In next theorem, we present conditions on the parameters𝑎1, 𝑎2, 𝑏1, 𝑏2, 𝑐1, 𝑐2and obtain a characterization for operator Ω which maps𝑇 𝐺𝐻(𝛾) onto itself.

Theorem 2.6. Let 𝑎𝑗, 𝑏𝑗 >0, 𝑐𝑗 > 𝑎𝑗+𝑏𝑗 for (𝑗= 1,2) and𝛾(0≤𝛾 <1).Then

Ω (𝑇 𝐺𝐻(𝛾))⊂𝑇 𝐺𝐻(𝛾), if and only if

𝐹(𝑎1, 𝑏1;𝑐1; 1) +𝐹(𝑎2, 𝑏2;𝑐2; 1)≤2.

Proof. Let𝑓 =ℎ+𝑔 ∈𝑇 𝐺𝐻(𝛾) with ℎand 𝑔 in (1.4). In view of Remark 1, we

only need to prove that Ω(𝑓) given by (1.3) is in𝑇 𝐺𝐻(𝛾), if and only if𝑃2≤1−𝛾, where

𝑃2=

𝑛=2

(2𝑛−1−𝛾)

(𝑎1)𝑛−1(𝑏1)𝑛−1

(𝑐1)𝑛−1(1)𝑛−1 𝐴𝑛

+

𝑛=1

(2𝑛+ 1 +𝛾)

(𝑎2)𝑛−1(𝑏2)𝑛−1

(𝑐2)𝑛−1(1)𝑛−1 𝐵𝑛

.

Using the coefficient estimates stated in Remark 1, we obtain

𝑃2≤(1−𝛾) [

𝑛=2

𝐷𝑛−1+

𝑛=1 𝐸𝑛−1

]

≤(1−𝛾) [𝐹(𝑎1, 𝑏1;𝑐1; 1)−1 +𝐹(𝑎2, 𝑏2;𝑐2; 1)]

≤(1−𝛾),

by the given condition.

(9)

References

[1] O.P. Ahuja, Planar harmonic univalent and related mappings, J. Inequal. Pure Appl. Math.,

6(4) (2005), Art. 122, 1-18.

[2] O.P. Ahuja, Planar harmonic convolution operators generated by hypergeometric functions, Integral Transform Spec. Funct.,18(3) (2007), 165-177.

[3] O.P. Ahuja, Connections between various subclasses of planar harmonic mappings involving hypergeometric functions, Appl. Math. Comput.,198(1) (2008), 305-316.

[4] O.P. Ahuja and J.M. Jahangiri, Noshiro-type harmonic univalent functions, Sci. Math. Jpn.,

6(2) (2002), 253-259.

[5] B.C. Carleson and D.B. Shaffer, Starlike and prestarlike hypergeometric functions, SIAM J. Math. Anal.,15(1984), 737-745.

[6] J . Clunie and T Sheil-Small, Harmonic univalent functions, Ann. Acad. Sci. Fen. Series A.I. Math.,9(1984), 3-25.

[7] P. Duren, Harmonic Mappings in the Plane, Cambridge Tracts in Mathematics, Vol.156, Cambridge University Press, Cambridge,2004, ISBN 0-521-64121-7.

[8] Y.E. Hohlov, Convolution operators preserving univalent functions, Ukrainian Math. J.,37

(1985), 220-226.

[9] S. Miller and P.T. Mocanu, Univalence of Gaussian and confluent hypergeometric functions, Proc. Amer. Math. Soc.,110(2) (1990), 333-342.

[10] S. Owa and H.M. Srivastava, Univalent and starlike generalized hypergeometric functions, Canad. J. Math.,39(1987), 1057-1077.

[11] S. Ponnusamy and F. Rønning, Starlikeness properties for convolution involving hypergeo-metric series, Ann. Univ. Mariae Curie-Sklodowska L.H.116(1998), 141-155.

[12] T. Rosy, B.A. Stephen, K.G. Subramanian and J.M. Jahangiri, Goodman-Rønning-type har-monic univalent functions, Kyungpook Math. J.,41(1) (2001), 45-54.

[13] S. Ruscheweyh and V. Singh, On the order of starlikeness of hypergeometric functions, J. Math. Anal. Appl.,113(1986), 1-11.

[14] A. Swaminathan, Certain Sufficiency conditions on Gaussian hypergeometric functions, J. Ineq. Pure Appl. Math.,5(4) (2004), Art. 83, 1-10.

[15] X.T. Wang, X.Q. Liang and Y.L. Zhang, Precise coefficient estimates for close-to-convex harmonic univalent mappings, J. Math. Anal. Appl.,263(2) (2001), 501-509.

Saurabh Porwal and K.K. Dixit

References

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