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Başlık: Univalence of certain integral operators involving normalized wright functionsYazar(lar):MUSTAFA, NizamiCilt: 66 Sayı: 1 Sayfa: 019-028 DOI: 10.1501/Commua1_0000000771 Yayın Tarihi: 2017 PDF

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UNIVALENCE OF CERTAIN INTEGRAL OPERATORS INVOLVING NORMALIZED WRIGHT FUNCTIONS

NIZAMI MUSTAFA

Abstract. In this paper our main aim is to give some su¢ cient conditions for functions represented with normalized Wright functions to be univalent in the open unit disk. The key tools in our proofs are the Becker’s and the generalized version of the well-known Ahlfor’s and Becker’s univalence criteria.

1. Introduction

Let A be the class of analytic functionsf (z) in the open unit disk U = fz 2 C : jzj < 1g, normalized by f(0) = 0 = f0(0) 1 of the form

f (z) = z + a2z2+ a3z3+ + anzn+ = z + 1

X

n=2

anzn: (1.1)

It is well-known that a function f : C ! C is said to be univalent if the following condition is satis…ed: z1 = z2 iff (z1) = f (z2). We denote by S the subclass of A

consisting of functions which are also univalent in U .

For some recent investigations of various subclasses of the univalent functions class S, see the works by Altinta¸s et al. [1], Gao et al. [7], and Owa et al. [8]. In recent years there have been many studies (see for example [2-6, 9, 10]) on the univalence of the following integral operators:

Gp(z) = p Z z 0 tp 1f0(t)dt 1=p ; (1.2) Gp;q(z) = p Z z 0 tp 1 f (t) t q dt 1=p (1.3) and Gq(z) = p Z z 0 tp 1 ef (t) q dt 1=p (1.4)

Received by the editors: March 18, 2016, Accepted: Aug 15, 2016. 2010 Mathematics Subject Classi…cation. 30C45, 33C10, 33E12.

Key words and phrases. Univalent function; Wright function; Becker’s univalence criteria.

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where the function f (z) belong to the class A and the parameters p; q are complex numbers such that the integrals in (1.2)-(1.4) exist. Furthermore, Breaz et al. [5] have obtained various su¢ cient conditions for the univalence of the following integral operator: Gn; (z) = 8 < :[n( 1) + 1] Z z 0 n Y k=1 fk(t) ! 1 dt 9 = ; 1=[n( 1)+1] (1.5) where n is a natural number, is a real number and functions fk 2 A; k =

1; :::; n: By Baricz and Frasin [2] was obtained some su¢ cient conditions for the univalence of the integral operators of the type (1.3)-(1.5) when the function f (z) is the normalized Bessel function with various parameters.

The Wright function is de…ned by the following in…nite series: W ; (z) = 1 X n=0 1 ( n + ) zn n! (1.6)

where is Euler gamma function, > 1; ; z 2 C. This series is absolutely convergent in C, when > 1 and absolutely convergent in open unit disk for = 1. Furthermore, for > 1 the Wright function W ; (z) is an entire function.

The Wright function was introduced by Wright in [12] and has appeared for the …rst time in the case > 0 in connection with his investigation in the asymptotic theory of partitions. Later on, it has found many other applications, …rst of all, in the Mikusinski operational calculus and in the theory of integral transforms of Hankel type. Furthermore, extending the methods of Lie groups in partial di¤erential equations to the partial di¤erential equations of fractional order it was shown that some of the group-invariant solutions of these equations can be given in terms of the Wright functions and of the integral operators involving Wright functions.

Note that Wright function W ; (z), de…ned by (1.6) does not belong to the class

A. Thus, it is natural to consider the following two kinds of normalization of the Wright function: W(1); (z) := ( )zW ; (z) = 1 X n=0 ( ) ( n + ) zn+1 n! ; > 1; > 0; z 2 U and W(2); (z) := ( + ) W ; (z) 1 ( ) = 1 X n=0 ( + ) ( n + + ) zn+1 (n + 1)!; > 1; + > 0; z 2 U: Easily, we write W(1); (z) = z + 1 X n=2 ( ) ( (n 1) + ) zn (n 1)!; > 1; > 0; z 2 U (1.7) and

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W(2); (z) = z + 1 X n=2 ( + ) ( n + ) zn n!; > 1; + > 0; z 2 U: (1.8) Note that W1;p+1(1) ( z) = Jp(1)(z) = (p + 1)z1 p=2Jp(2pz)

where Jp(z) is the Bessel function and Jp(1)(z) the normalized Bessel function.

In this paper, we give various su¢ cient conditions for integral operators of type (1.2)-(1.4) when the function f (z) is the normalized Wright functions to be univa-lent in the open unit disk U . We would like to show that the univalence of integral operators which involve normalized Wright functions can be derived easily via some well-known univalence criteria.

2. PRELIMINARIES

In this section, we give the necessary information and lemmas, which shall need in our investigation.

In our investigation, we shall need the following lemmas. Lemma 1([3]). If f 2 A and the following condition is satis…ed:

1 jzj2 zf00(z) f0(z) 1

for all z 2 U then the function f(z) is univalent in U.

Lemma 2 ([10]). Let q 2 C and a 2 R such that Re(q) 1; a > 1 and 2a jqj 3p3. If f 2 A satis…es the inequality jzf0(z)j a for all z 2 U then the function

Gq : U ! C de…ned by (1.4) univalent in U.

Lemma 3 ([9]). Let p and c be complex numbers such that Re(p) > 0 and jcj 1; c 6= 1. If the function f 2 A satis…es the inequality

c jzj2p+ (1 jzj2p)zf00(z) pf0(z) 1

for all z 2 U then the function Gp: U ! C de…ned by (1.2) is univalent in U.

We shall need, also the following results.

Lemma 4. Let 1 and > 0 where 0= 1:2581 is the root of the equation

2 ( + 1)e 1+1+ 1 = 0: (2.1)

Then, the following inequalities hold for all z 2 U z W(1); (z) 0 W(1); (z) 1 e1=( +1) (2 + 1) ( + 1)e1=( +1); (2.2) z W(1); (z) 0 1 + 1 n( + 2)e +11 ( + 1) o : (2.3)

Proof. By using the de…nition of the normalized Wright function W(1); (z), we obtain for all z 2 U

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z W(1); (z) 0 W(1); (z) 1 = z W(1); (z) 0 W(1); (z) W(1); (z) P1 n=2 ( ) ( (n 1)+ ) 1 (n 2)! 1 P1 n=2 ( ) ( (n 1)+ )(n11)! : Under hypothesis 1, the inequality (n 1 + ) ( (n 1) + ); n 2 N holds, which is equivalent to

( ) ( (n 1) + ) 1 ( )n 1; n 2 N (2.4) where ( )n = (n + )= ( ) = ( + 1) ( + n 1); ( )0= 1 is Pochhammer

(or Appell) symbol, de…ned in terms of Euler gamma function. Using (2.4), we obtain 1 X n=2 ( ) ( (n 1) + ) 1 (n 2)! 1 X n=2 1 (n 2)! 1 ( )n 1 : Further, the inequality

( )n 1= ( + 1) ( + n 2) ( + 1)n 2; n 2 N (2.5)

is true, which is equivalent to 1=( )n 1 1= ( + 1)n 2; n 2 N. Using (2.5), we

get 1 X n=2 ( ) ( (n 1) + ) 1 (n 2)! 1 X n=2 1 (n 2)! 1 ( + 1)n 2 = e1=( +1) : (2.6) Similarly, we have 1 X n=2 ( ) ( (n 1) + ) 1 (n 1)! + 1 e1=( +1) 1 : (2.7)

Combining inequalities (2.6) and (2.7), we immediately get that …rst assertion (2.2) of Lemma 4 holds.

Let’s prove second assertion of lemma. From the de…nition of the normalized Wright function W(1); (z), we have

z W(1); (z)

0

1 +P1n=2(n 2)!1 ( (n 1)+ )( ) +P1n=2(n 1)!1 ( (n 1)+ )( ) : Using (2.6) and (2.7), we get

z W(1); (z) 0 1 + e 1=( +1) + + 1 e1=( +1) 1 = 1 + 1 h( + 2)e1=( +1) ( + 1)i: Thus, the proof of Lemma 4 is complete.

For the normalized Wright function W(2); (z), we can give the following lemma. Lemma 5. Let 1 and + > x0 where x0= 1:2581 is the root of the equation

2x (x + 1)ex+11 + 1 = 0: (2.8)

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z W(2); (z) 0 W(1); (z) 1 ( + + 1) e1=( +1) 1 ( + ) ( + + 1) e1=( +1) 1 ; (2.9) z W(2); (z) 0 1 + + + 1 + e 1=( +1) 1 : (2.10)

Proof. The proof of this lemma is very similar to the proof of Lemma 4, so the details of the proof may be omitted.

3. UNIVALENCE OF INTEGRAL OPERATORS INVOLVING WRIGHT FUNCTIONS

In this section our main aim is to give su¢ cient conditions for the integral op-erators of the type (1.2)–(1.4) when the function f (z) is the normalized Wright functions to be univalent in the open unit disk U . To this end, …rstly we consider the following integral operator:

Gq; (z) = Z z 0 W(1); (t) t !q dt; > 1; > 0; z 2 U: (3.1) For this integral operator, we can give the following theorem.

Theorem 1. Let 1 and > 0 where 0= 1:2581 is the root of the equation (2.1). Moreover, suppose that q is a complex number such that

jqj (2 + 1) ( + 1)e

1=( +1)

e1=( +1) :

Then, the function Gq; : U ! C de…ned by (3.1) is univalent in U. Proof. Since W(1); 2 A, clearly Gq; 2 A, i. e. Gq; (0) = Gq; (0)

0

1 = 0. On the other hand, it is easy to see that

Gq; (z) 0 = W (1) ; (z) z !q and z Gq; (z) 00 Gq; (z) 0 = q 2 6 4 z W(1); (z) 0 W(1); (z) 1 3 7 5 : (3.2)

By using …rst assertion (2.2) of Lemma 4, we obtain z Gq; (z) 00 Gq; (z) 0 jqj z W(1); (z) 0 W(1); (z) 1 jqj e1=( +1) (2 + 1) ( + 1)e1=( +1)

for all z 2 U and > 0 where 0= 1:2581 is the root of the equation (2 + 1) ( + 1)e +11 = 0:

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(1 jzj2) z Gq; (z) 00 Gq; (z) 0 (1 jzj 2 ) jqj e 1=( +1) (2 + 1) ( + 1)e1=( +1):

This last expression is bounded by 1 if

jqj (2 + 1) ( + 1)e

1=( +1)

e1=( +1) :

But, this is true by hypothesis of theorem. Thus, according to the Lemma 1, function Gq; (z) is univalent in U . With this the proof of Theorem 1 is complete. By setting q = 1 in Theorem 1, we have the following result.

Corollary 1. Let 1 and > 1 where 1= 2:4898 is the root of the equation

(2 + 1) ( + 2)e +11 = 0: (3.3)

Then, the unction G ; : U ! C de…ned by

G ; (z) = Z z 0 W(1); (t) t dt is univalent in U .

If we take = 1; = p + 1 in Theorem 1, we arrive at the following corollary. Corollary 2. The function Gq

p: U ! C de…ned by Gqp(z) = Z z 0 Jp(1)( t) t !q dt

is univalent in U if p > 0 1 where 0= 1:2581 is the root of the equation (2.1) and q is a complex number such that

jqj (2p + 3) (p + 2)e

1=(p+2)

e1=(p+2)

Here, function Jp(1)(z) is normalized Bessel function.

By taking q = 1 in Corollary 2, we obtain the following result.

Corollary 3. Let p > 1 1 where 1= 2:4898 is the root of the equation (3.3). Then, the function Gp: U ! C de…ned by

Gp(z) =

Z z 0

Jp(1)( t)

t dt

is univalent in U . Here, Jp(1)(z) is normalized Bessel function.

For the integral operator Fq; (z) = Z z 0 W(2); (t) t !q dt; > 1; + > 0; z 2 U (3.4) we can give the following theorem.

Theorem 2. Let 1 and + > x0 where x0 = 1:2581 is the root of the

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jqj ( + ) ( + + 1) e

1=( +1) 1

( + + 1) e1=( +1) 1 :

Then, the function Fq; : U ! C de…ned by (3.4) is univalent in U.

Proof. The proof of this theorem is very similar to the proof of Theorem 1, so the details of the proof may be omitted.

By setting q = 1 in Theorem 2, we have the following corollary.

Corollary 4. Let 1 and + > x1 where x1 = 2:3325 is the root of the

equation

3x 2(x + 1)ex+11 + 2 = 0: (3.5)

Then, the function F ; : U ! C de…ned by

F ; (z) = Z z 0 W(2); (t) t dt is univalent in U .

Now, we consider the following integral operator: Gp;q; (z) = 8 < :p Z z 0 tp 1 W (1) ; (t) t !q dt 9 = ; 1=p ; > 1; > 0; z 2 U: (3.6) On the univalence of the function Gp;q; (z), we give the following theorem.

Theorem 3. Let 1 and > 0 where 0= 1:2581 is the root of the equation (2.1). Moreover, suppose that p; q and c be complex numbers such that Re(p) > 0; jcj < 1 and the following condition is satis…ed:

jcj 1 jqj e

1=( +1)

jpj (2 + 1) ( + 1)e1=( +1) :

Then, the integral operator Gp;q; : U ! C de…ned by (3.6) is univalent in U. Proof. We can rewrite the integral operator (3.6) as

Gp;q; (z) = p Z z 0 tp 1 Gq; (t) 0 dt 1=p (3.7) where function Gq; : U ! C is de…ned in (3.1).

Under hypothesis of theorem, using (3.2) and (2.2), we obtain c jzj2p+ (1 jzj2p) z Gq; (z) 00 p Gq; (z) 0 jcj + jqj e1=( +1) jpj (2 + 1) ( + 1)e1=( +1) :

This last expression is bounded by 1 if

jcj 1 jqj e

1=( +1)

jpj (2 + 1) ( + 1)e1=( +1) :

But this is true by hypothesis of theorem. Thus, according to the Lemma 3, function Gp;q; (z) de…ned by (3.7) is univalent in U . With this, the proof of Theorem 3 is complete.

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Corollary 5. Let 1 and > 0 where 0 = 1:2581 is the root of the equation (2.1). Moreover, suppose that p and c be complex numbers such that Re(p) > 0; jcj < 1 and the following condition is satis…ed:

jcj 1 e

1=( +1)

jpj (2 + 1) ( + 1)e1=( +1) :

Then, the integral operator Gp; : U ! C de…ned by Gp; (z) = p Z z 0 tp 2W(1); (t)dt 1=p : (3.8) is univalent in U .

Remark 1. Note that, recently the function Gp; : U ! C de…ned by (3.8) was investigated by Prajapat [11] and he obtained some su¢ cient conditions for the univalence this function.

Now, on the univalence of the integral operator Fp;q; (z) = 8 < :p Z z 0 tp 1 W (2) ; (t) t !q dt 9 = ; 1=p ; > 1; + > 0; z 2 U (3.9) we can give the following theorem.

Theorem 4. Let 1 and + > x0 where x0 = 1:2581 is the root of the

equation (2.8). Moreover, suppose that p; q and c be complex numbers such that Re(p) > 0; jcj < 1 and the following condition is satis…ed:

jcj 1 jqj ( + + 1) e

1=( +1) 1

jpj ( + ) ( + + 1) e1=( +1) 1 :

Then, the integral operator Fp;q; : U ! C de…ned by (3.9) is univalent in U. Proof. The proof of Theorem 4 is similar to the proof of Theorem 3. Hence, the details of the proof of Theorem 4 may be omitted.

By setting q = 1 in Theorem 4, we obtain the following corollary.

Corollary 6. Let 1 and + > x0 where x0 = 1:2581 is the root of

the equation (2.8). Moreover, suppose that p and c be complex numbers such that Re(p) > 0; jcj < 1 and the following condition is satis…ed:

jcj 1 ( + + 1) e

1=( +1) 1

jpj ( + ) ( + + 1) e1=( +1) 1 :

Then, the function Fp; : U ! C de…ned by Fp; (z) = p Z z 0 tp 2W(2); (t)dt 1=p ; z 2 U (3.10) is univalent in U .

Now, we consider integral operator of the type (1.4) when the function f (z) is the normalized Wright function.

Let Hq; (z) = q Z z 0 tq 1 eW(1); (t) q 1=q ; > 1; + > 0; z 2 U: (3.11)

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On univalence of the function (3.11), we give the following theorem.

Theorem 5. Let q 2 C; 1 and > 0 where 0 = 1:2581 is the root of the equation (2.1). If Re(q) 1 and the following condition is satis…ed:

jqj 3

p 3

2 ( + 2)e1=( +1) 1 (3.12)

then the function Hq; : U ! C de…ned by (3.11) is univalent in U. Poof. From (2.3), we write

z W(1); (z)

0

1 + 1 n( + 2)e +11 ( + 1)

o for all z 2 U. Taking

a = 1 + 1 n( + 2)e 1+1 ( + 1)

o ;

we easily see that 2a jqj 3p3 if provided (3.12). Thus, under hypothesis of theorem, all hypothesis of the Lemma 2 is provided. Hence, the proof of Theorem 5 is complete.

By setting q = 1 in Theorem 5, we have the following result.

Corollary 7. Let 1 and > 1 where 1= 1:6692 is the root of the equation

3p3 2( + 2)e1=( +1)+ 2 = 0: (3.13)

Then, the function H ; : U ! C de…ned by

H ; (z) = Z z 0 eW(1); (t)dt is univalent in U . Now, let Qq; (z) = q Z z 0 tq 1 eW(2); (t) q 1=q ; > 1; + > 0; z 2 U: (3.14) For the function (3.14), we can give the following theorem which will be proved similarly to the Theorem 5.

Theorem 6. Let q 2 C; 1 and + > x0 where x0 = 1:2581 is the root of

the equation (2.1). If Re(q) 1 and the following condition is satis…ed:

jqj 3

p

3( + )

2 ( + + 1)e1=( + +1) 1

then the function Qq; : U ! C de…ned by (3.14) is univalent in U. By setting q = 1 in Theorem 6, we obtain the following corollary.

Corollary 8. Let 1 and + > x1 where x1 = 0:83232 is the root of the

equation

3p3x 2(x + 1)e1=(x+1)+ 2 = 0: Then, the function Q ; : U ! C de…ned by

Q ; (z) =

Z z 0

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is univalent in U .

References

[1] Altinta¸s, O., Irmak, H., Owa, S., Srivastava, H. M., Coe¢ cient bounds for some families of starlike and convex functions of complex order, Applied Mathematics Letters 20 (2007), 1218-1222.

[2] Baricz, A., Frasin, B. A., Univalence of integral operators involving Bessel functions, Applied Mathematics Letters, 23 (2010), 371-376.

[3] Becker, J., Löwnersche Di¤erentialgleichung und quasikonform fortsetzbare schlichte Funk-tionen, J. Reine Angew Math. 255 (1972), 23-43 (in German).

[4] Blezu, D., On Univalence Criteria, General Mathematics, 14 2006, 87-93.

[5] Breaz, D., Breaz, N., Srivastava, H. M., An extension of the univalent condition for a family of integral oprator, Applied Mathematics Letters, 22 (2009), 41-44.

[6] Breaz, D., Günay, H. Ö., On the univalence criterion of a general integral operator, J. Inequal. Appl. 8 (2008), Art. ID 702715.

[7] Gao, C.-Y., Yuan, S.-M., Srivastava,H. M., Some functional inequalities and inclusion re-lationships associated with certain families of integral operators, Comput. Math. Appl. 49 (2015), 1787-1795.

[8] Owa, S., Nunokawa, M., Saitoh, H., Srivastava, H. M., Close-to-convexity, starlikeness and convexity of certain analytic functions, Appl. Math. Lett. 15 (2002), 63-69.

[9] Pescar, V., A new generalization of Ahlfor’s and Becker’s criterion of univalence, Bull. Math. Soc. (Second Series), 9 (1996), 53-54.

[10] Pescar, V., Univalence of certain integral operators, Acta Univ. Apulensis Math. Infom., 12 (2006), 43-48.

[11] Prajapat, J. K., Certain geometric properties of the Wright function. Integral Transform and Special Functions, 26 (2015), 203-212.

[12] Wright, E. M., On the coe¢ cients of power series having exponential singularities, J. London Math. Soc. 8 (1933), 71-79.

Current address : N. Mustafa: Department of Mathematics, Faculty of Science and Letters, Kafkas University, Kars, 36100, Turkey.

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