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Some Properties of the Class of Univalent Functions

with Negative Coefficients

Aisha Ahmed Amer, Maslina Darus*

School of Mathematical Sciences, Faculty of Science and Technology, Universiti Kebangsaan Malaysia, Bangi, Malaysia

Email: [email protected], *[email protected]

Received August 6, 2012; revised October 17, 2012; accepted October 26, 2012

ABSTRACT

The main object of this paper is to study some properties of certain subclass of analytic functions with negative coeffi- cients defined by a linear operator in the open unit disc. These properties include the coefficient estimates, closure properties, distortion theorems and integral operators.

Keywords: Analytic Function; Unit Disc; Coefficient Inequality; Closure Properties; Distortion Bound

1. Introduction

Let be the class of analytic functions in the open unit disc

: 1

Uz z  ,

and 

 

a n, be the subclass of consisting of func- tions of the form

 

1

1 .

n n

n n

f z  a a za z  

Let 

 

n denote the class of functions f z

 

nor- malized by

 

1

, : 1, 2, 3,

k k k n

f z z a z n

 

 

  

, (1)

which are analytic in the open unit disc. In particular,

 

1 : .

 

For two functions f z

 

given by (1) and g z

 

given by

 

1

, ,

k k k n

g z z b z n

 

 



the Hadamard product (or convolution)

fg

 

z is defined, as usual, by

 



1

: k k k:

k n

.

f g z z a b z g f z

 

  

 

Let the function 

a b z, ;

be given by:

 

 

1

1 1

, ; k k, 0, 1, 2, 3, ,

k n k

a

a b z z z b

b

  

 

 

    

where

 

x k denotes the Pochhammer symbol (or the shifted factorial) defined by:

 

 

1

for 0,

 

1 1 for 1, 2, 3

k

k x

x

x x x k k

 

     



 

0 ,

, .

  

Carlson and Shaffer [1] introduced a convolution operator on involving an incomplete beta function as:

   

, :

, ;

  

L a b f z  a b zf z . (2)

Our work here motivated by Catas [2], who introduced an operator on  as follows:

 

,

1

1 1

, 1

m

m k

l k

k n

k l

D f z z a z

l

  

 

  

 

 

 

where

, 0, , 0

z m l .

Now, using the Hadamard product (or convolution), the authors (cf. [3,4]) introduced the following linear operator:

Definition 1.1 Let

 

 

, 1

1 1

1 1

, ; ,

1

m

m k k

l

k n k

a

k l

a b z z

l b

 

  

 

  

 

  

 

where

zU b,    0, 1, 2, 3,

,0,m,l0, and

 

x k is the Pochhammer symbol. We defines a linear operator Dlm,

   

a b, : n 

n

by the fol- lowing Hadamard product:
(2)

   

  

 

 

, ,

1

1 1

, : , ;

1 1

, 1

m m

l l

m

k k

k

k n k

D a b f z a b z f z

a k l

z a

l b

 

 

  

 

  

 

z (3)

where

zU b,    0, 1, 2, 3,

,0,m,l0, and

 

x k the Pochhammer symbol .

Special cases of this operator include:

 ,0

   

0,

   

   

0 , , ,

m

l

D a b f zDa b f zL a b f z , see [1].

 the Catas drivative operator [2]: ,

   

1,1 .

m l

Df z

 the Ruscheweyh derivative operator [5] in the cases:

  

 

0,0

0 1,1 ; 1.

D  f zD f z  

 the Salagean derivative operator [6]: ,1

   

0 1,1 .

m

D f z

 the generalized Salagean derivative operator intro- duced by Al-Oboudi [7]: ,

   

z

0 1,1 .

m

Df

 Note that:

   

   

   

   

   

   

0, 0 1,

, , ,

1

, ,

1

, , , 0

1

l

D a b f z L a b f z

l

D a b f z L a b f z l

z

L a b f z D L a b f z l

  

 

 

  

 .

Let 

 

n denote the class of functions f z

 

of the form

1

( ) k k, k 0, ,

k n

f z z a z a n

 

 

  (4)

which are analytic in the open unit disc.

Following the earlier investigations by [8] and [9], we define

n,

-neighborhood of a function f z

 



 

n

by

 

 

 

,

1 1

:

n

k

k k

k n k n

N f

g z z b z n k a b

k

 

   

 

     

or,

 

 

 

,

1 1

: k :

n k

k n k n

Nh g z z b z n k bk  ,

 

   

 

   

where h z

 

z.

 

Let n

 denote the subclass of consisting

of functions which satisfy

 

n

 

 

Re zf z ,z U, 0 1.

f z  

 

   

 

 

 

A function f z

 

in n

 

 is said to be starlike of order  in U.

A function f z

 



 

n is said to be convex of order  it it satisfies

 

 

Re 1 zf z ,z U, 0 1.

f z  



 

    

 

 

We denote by n

 

 the subclass of 

 

n con-

sisting of all such functions [10]. The unification of the classes n

 

 and n

 

 is

provided by the class n

 ,

of functions

 

 

f z  n which also satisfy the following inequality

 

 

  

  

2

Re ,

1

, 0 1, 0 1.

zf z z f z zf z f z

z U

 

      

 

 

 

    

The class n

 ,

was investigated by Altintas [11]. Now, by using Dlm,

 

a b, we will define a new class of starlike functions.

Definition 1.2 Let

0 1, 0 1,

0, 1, 2, 3, , , 0, 0.

b m l

 

   

       

A function f belonging to is said to be in the class

 

n

, , , , ,

m

l n a

  

b if and only if

   

   

   

   

, 1,

, 1,

1 , ,

Re

1 , ,

, .

m m

l l

m m

l l

z D a b f z z D a b f z

z D a b f z z D a b f z

z U

 

 

 

 

 



 

 

 

 

 

 

(6)

Remark 1.3 The class is a genera- lization of the following subclasses:

, , , , ,

m

l n a

  

b

i) 1,00

1, , 0,1,1

 

 1

 

 

    and

1, , 0,1,1

 

 

1

1,0     1 

   defined and studied by

[12];

ii) 1,00

1, , 0,1,1

and studied by

[13] and [14];

1

1,0 1, , 0,1,1

iii) 1,0

1, , 0,1,1

,

m   m

  studied by [15];

iv) 1,00

n, , ,1,1 

Now, we shall use the same method by [17] to estab- lish certain coefficient estimates relating to the new introduced class.

studied by [16].

2. Coefficient Estimates

Theorem 2.1 Let the function f be defined by (1). Then f belongs to the class if and only if

n, , , ,  a

,

m l

b



1



, , , , 1 1

1 1 ,

k k

k n

c m l a b k l k a

l

  

  

     

  

(7)

(3)

 



1



1

,

, , , , 1 1

1.

k k

k

l

f z z z

c m l a b k l k

k n

  

 

 

     

 

(9)

 

 

11

, , , ,

1 1

. 1

k

m k k

c m l a b

a

k l

l b

  

 

 

 

(8)

Proof: Assume that the inequality (7) holds and let 1

z  . Then we have The result is sharp and the extremal functions are

   

   

   

   

  

  

  

 

, 1,

, 1,

1 1

1 1

1 1

1 1

1

1 , ,

1

1 , ,

1 1 1 1

1

1 1

1 1 1 1

1

1 1

1 1

1

m m

l l

m m

l l

m

k k

k

k n k

m

k k

k

k n k

k n

z D a b f z z D a b f z

z D a b f z z D a b f z

a

k l l k

k a z

l l b

a

k l l k

a z

l l b

k l

 

 

 

 

 

 

 

 

 

 

 

 

 

 

     

   

 

   

     

   

 

 

   

  

 

  

 

  

 

1 1

1

1 1

1 1

1

1 1

1 .

1 1 1 1

1

1 1

m

k k k m

k k

k n k

a l k

ka

l l b

a

k l l k

a

l l b



 

 

 

  

   

 

     

     

   

 

 

   

Consequently, by the maximum modulus theorem one obtains

Conversely,suppose that

 

,

, , , ,

m l

f z  n  ab .

 

,

, , , ,

.

m l

f z  n  a b

Then from (6) we find that

  

 

  

 

1

1 1

1

1 1

1 1 1 1

1 1

Re .

1 1 1 1

1 1

m

k k

k

k n k

m

k k

k

k n k

a

k l l k

z k

l l b

a

k l l k

z a

l l b

 

a z

z

 

 

 

     

   

 

     

 

     

   

   

   

 

Choose values of z on the real axis such that

   

   

   

   

, 1,

, 1,

1 , ,

1 , ,

m m

l l

m m

l l

z D a b f z z D a b f z

z D a b f z z D a b f z

 

 

 

 

 

 

 

is real. Letting z1 through real values, we obtain

  

 

  

 

1

1 1

1

1 1

1 1 1 1

1

1 1

Re ,

1 1 1 1

1

1 1

m

k k

k n k

m

k k

k n k

a

k l l k

ka

l l b

a

k l l k

a

l l b

 

 

 

 

     

   

 

 

 

     

   

   

   

 

or, equivalently

  

 

  

 

1

1 1

1

1 1

1 1 1 1

1

1 1

1 1 1 1

1 ,

1 1

m

k k

k n k

m

k k

k n k

a

k l l k

ka

l l b

a

k l l k

a

l l b

 

 

 

 

     

   

 

 

   

     

 

 

 

   

 

 

(4)

which gives (7).

Remark 2.2 In the special case Theorem

2.1 yields a result given earlier by [17]. 1,

a b

Remark 2.3 In the special case 1, 0,l

Theorem 2.2 yields a result given earlier by

[6]. 1,

a b

Theorem 2.4 Let the function f defined by (3) be in the class ,

, , , ,

. Then

m

l n a

  

b







1 1

1 1

,

, , , , 1 1

k

k n n

l a

c m l a b l n n

  

  

 

   

(10)

and









1 1

1 1 1

.

, , , , 1 1

k

k n n

l n

ka

c m l a b l n n

  

  

   

   

(11)

The equality in (10) and (11) is attained for the func- tion f given by (9).

Proof: By using Theorem 2.2, we find from (6) that







1

1 1

1 1 , , , ,

, , , , 1 1

1 1 ,

n k

k n

k k

k n

l n n c m l a b a

c m l a b k l k a

l

  

  

 

  

 

   

     

  

,

a

which immediately yields the first assertion (10) of Theorem 2.3.

On the other hand, taking into account the inequality (6), we also have



1

1

1 , , , ,

1 1 ,

n k

k n

l n c m l a b k a

l

  

 

 

  

  

that is



1

1 1

1

1 , , , ,

1 1 1 , , , ,

n k

k n

n k

k n

l n c m l a b ka

l l n c m l a b

 

   

 

 

 

   

     

which, in view of the coefficient inequality (10), can be put in the form









1

1 1

1

1 , , , ,

1 1 1 , , , ,

1 1

,

, , , , 1 1

n k

k n

n

n

l n c m l a b ka

l l n c m

l

c m l a b l n n

 

   

  

 

 

  

     

 

   

l a b

and this completes the proof of (11).

3. Closure Theorem

Theorem 3.1 Let the function fj

  

z , j1, 2,,m

be defined by

 

1

,

k

j k

k n j f z z a z

 

 

for zU, be in the class then the

function

, , , , ,

m

l n a

  

b

 

h z defined by

 

1

, 0

k

k kj

k n

h z z b z a ,

  

 

also belongs to the class ,

, , , ,

, where

m

l n a

  

b

1 m

.

k j n kj

b a

m  

Proof: Since

 

,

, , , , , m

j l

f z  n  ab

j

it follows from Theorem 2.1, that



1



 

, , , , 1 1

1 1 , 1, 2, , .

k k

k n

c m l a b k l k a

l j m

  

 

     

   

Therefore,









1

1

1

, , , , 1 1

1

, , , , 1 1

1

, , , , 1 1

1 1 .

k k

k n

m

k k

k n j n

m

k k

j n k n

c m l a b k l k b

c m l a b k l k a

m

c m l a b k l k a m

l

  

  

  

j

j

  

  

  

     

            

 

     

 

  

 

Hence by Theorem 2.1,

 

,

, , , ,

also.

m l

h z  n  a b

Morever, we shall use the same method by [17] to prove the distrotion Theorems.

4. Distortion Theorems

Theorem 4.1 Let the function f defined by (1) be in the class ,

, , , ,

m

l n a

  

b . Then we have

   







,

1

,

1 1

,

, , , , 1 1

i l

n

k D a b f z

l

z z

c m i l a b n l n

  

   

    

(12)

and

   







,

1

,

1 1

,

, , , , 1 1

i l

n

k D a b f z

l

z z

c m i l a b n l n

  

   

    

(13)

for zU, where 0 i m and is

given by (8).

, , , ,

k

c m i  l a b

The equalities in (12) and (13) are attained for the function f given by

 



 



1

1

1

1 1

.

1 1 1

n

m

n m

f z

l

z z

n l n l n

  

   

     

(5)

Proof: Note that ,

, , , ,

m

l

f n  ab if and only if

   

,

,

,

i

l l

Da b f z m in, , , ,  a b , where

   

,

1

, , , ,

i k

l k

k n

Da b f z z c il a b a z

 

 

, k .

By Theorem 2.2, we know that







1 1

, , , , 1

1 , , , ,

, , , , 1 1

1 1 ,

k

k k

k n

k k

k n

c m i l a b n

l n c i l a b a

c m l a b k l k a

l

 

 

  

   

 

  

  

     

  

that is







1

, , , ,

1 1

.

, , , , 1 1

k k

k n

k

c i l a b a

l

c m i l a b n l n

 

 

  

    



The assertions of (12) and (13) of Theorem 4.1 follow immediately. Finally, we note that the equalities (12) and (13) are attained for the function f defined by

   







,

1

,

1 1

.

, , , , 1 1

i l

n

k D a b f z

l z

c m i l a b n l n

   z

   

    

This completes the proof of Theorem 4.1.

Remark 4.2 In the special case Theorem

4.1 yields a result given earlier by [17].

1,

a b

Corollary 4.3 Let the function f defined by (1) be in the class ,

, , , ,

m

l n a

  

b . Then we have

 



, , , ,1



11



1

1,

n

k f z

l

z z

c m l a b n l n

  

   

   

(15)

and

 



, , , ,1



11



1

1,

n

k f z

l

z z

c m l a b n l n

  

   

   

(16)

for . The equalities in (15) and (16) are attained for the function

zU

1 n

f  given in (14).

Corollary 4.4 Let the function f defined by (1) be in the class ,

, , , ,

m

l n a

  

b . Then we have

 









1 1 1

1

, , , , 1 1

n

k f z

l n

z c m l a b n l n

  

    

   

and

 









1 1 1

1 ,

, , , , 1 1

n k

f z

l n

z

c m l a b n l n

  

  

 

   

(18)

for zU. The equalities in (17) and (18) are attained for the function fn1 given in (14).

Corollary 4.5 Let the function f defined by (3) be in the class ,

, , , ,

m

l n a

  

b . Then the unit disc is mapped onto a domain that contains the disc





 







, , , , 1 1 1 1

.

, , , , 1 1

k

k

w

c m l a b n l n l

c m l a b n l n

   

  

      

   

The result is sharp with the extremal function fn1

given in (14).

5. Integral Operators

Theorem 5.1 Let the function f z

 

defined by (1) be in the class ,

, , , ,

m

l n  a

1.

c  b

 

and let be a real

number such that Then

c

,

F z defined by

 

1

 

0

1

d ,

z c c c

F z t f t z

t

b

also belongs to the class ,

, , , ,

m

l n a

  

Proof: From the representation of F z

 

, it is ob- tained that

 

1

, ,

k k k n

F z z b z n

 

 



where

1 .

k k

c

b a

k c

 

  Therefore









1 1

1

, , , , 1 1

1

, , , , 1 1

, , , , 1 1

1 1 ,

k k

k n

k k

k n

k k

k n

c m l a b k l k b

c

c m l a b k l k a

k c

c m l a b k l k a

l

  

  

  

  

  

  

     

 

       

 

      

  

since f z

 

belongs to so by virtue

of Theorem 2.1,

, , , , ,

m

l n a

  

b

 

F z is also element of

, , , , ,

m

l n a

  

b

, (17)

6. Acknowledgements

(6)

REFERENCES

[1] B. C. Carlson and D. B. Shaffer, “Starlike and Prestarlike Hypergeometric Functions,” SIAM Journal on Mathe- matical Analysis, Vol. 15, No. 4, 1984, pp. 737-745.

doi:10.1137/0515057

[2] A. Catas, “On a Certain Differential Sandwich Theorem Associated with a New Generalized Derivative Operator,” General Mathematics, Vol. 17, No. 4, 2009, pp. 83-95. [3] A. A. Amer and M. Darus, “A Distortion Theorem for a

Certain Class of Bazilevic Function,”International Jour- nal of Mathematical Analysis, Vol. 6, No. 12, 2012, pp. 591-597.

[4] A. A. Amer and M. Darus, “On a Property of a Subclass of Bazilevic Functions,” Missouri Journal of Mathemati- cal Sciences, In Press.

[5] St. Ruscheweyh, “New Criteria for Univalent Functions,” Proceedings of the American Mathematical Society, Vol. 49, No. 1, 1975, pp. 109-115.

[6] G. S. Salagean, “Subclasses of Univalent Functions,” Lecture Notes in Mathematics, Vol. 1013, 1983, pp. 362- 372. doi:10.1007/BFb0066543

[7] F. M. Al-Oboudi, “On Univalent Functions Defined by a Generalized Salagean Operator,” International Journal of Mathematics and Mathematical Sciences, Vol. 2004, No. 27, 2004, pp. 1429-1436.

doi:10.1155/S0161171204108090

[8] A. W. Goodman, “Univalent Functions and Nonanalytic Curves,” Proceedings of the American Mathematical So- ciety, Vol. 8, No. 3, 1957, pp. 598-601.

doi:10.1090/S0002-9939-1957-0086879-9

[9] St. Ruscheweyh, “Neighborhoods of Univalent Functions,” Proceedings of the American Mathematical Society, Vol.

81, No. 4, 1981, pp. 521-527.

doi:10.1090/S0002-9939-1981-0601721-6

[10] O. Alintas, H. Irmak and H. M. Srivastava, “Fractional Calculus and Certain Starlike Functions with Negative Coefficietns,” Computers & Mathematics with Applica- tions,Vol. 30, No. 2, 1995, pp. 9-15.

doi:10.1016/0898-1221(95)00073-8

[11] O. Alintas, “On a Subclass of Certain Starlike Functions with Negative Coefficients,” Journal of the Mathematical Society of Japan, Vol. 36, 1991, pp. 489-495.

[12] H. Silverman, “Univalent Functions with Negative Coef- ficients,” Proceedings of the American Mathematical So- ciety, Vol. 51, No. 1, 1975, pp. 109-116.

doi:10.1090/S0002-9939-1975-0369678-0

[13] S. K. Chatterjea, “On Starlike Functions,” Journal of Pure Mathematics, Vol. 1, 1981, pp. 23-26.

[14] H. M. Srivastava, S. Owa and S. K. Chatterjea, “A Note on Certain Classes of Starlike Functions,” Rendiconti del Seminario Matematico della Università di Padova, Vol. 77, 1987, pp.115-124.

[15] M. D. Hur and G. H. Oh, “On Certain Class of Analytic Functions with Negative Coefficients,” Pusan Kyongnam Mathematical Journal, Vol. 5, No. 1, 1989, pp. 69-80. [16] M. Kamali, “Neighborhoods of a New Class of p-Valently

Functions with Negative Coefficients,” Mathematical Inequalities & Applications,Vol. 9, No. 4, 2006, pp. 661- 670. doi:10.7153/mia-09-59

doi:10.1137/0515057 doi:10.1007/BFb0066543 doi:10.1155/S0161171204108090 doi:10.1090/S0002-9939-1957-0086879-9 doi:10.1090/S0002-9939-1981-0601721-6 doi:10.1016/0898-1221(95)00073-8 doi:10.1090/S0002-9939-1975-0369678-0 670. doi:10.7153/mia-09-59

References

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