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ON SOME PROPERTIES OF A GENERALIZED CLASS OF CLOSE-TO-STARLIKE FUNCTIONS

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ON SOME PROPERTIES OF A GENERALIZED CLASS OF

CLOSE-TO-STARLIKE FUNCTIONS

Ajab Bai Akbarally1 and Nor Siti Khadijah Arunah2

Faculty of Computer and Mathematical Sciences

1Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia

2Universiti Teknologi MARA Cawangan Johor, Kampus Segamat, 85000 Segamat, Johor,

Malaysia

1[email protected], 2[email protected]

ABSTRACT

In this paper, we consider a new class of close-to-starlike functions denoted byCS,, defined by the Carlson-Shaffer operatorL

,

. Let Sdenote the class

of analytic univalent functions

f

defined by

 

 

2 ,

n n nz

a z z

f then fCS,

if

f

satisfy the condition

 

  

z E z

g z

f

   

 

, 0 ,

Re L  , where

  

 

 

 

 

2 1

1 ,

n

n n n n a z

z z f

  

L and g(z) is a starlike function. Properties of

the class CS, such as the coefficient bounds, growth and distortion theorems and radius results are investigated.

Keywords: close-to-starlike functions, analytic functions, starlike functions, Carlson-Shaffer operator, coefficient bound, growth and distortion theorems, radius results.

1. Introduction

Let A denote the class of functions of the form

 

 

2

n n nz

a z z

f (1.1)

that are analytic and normalized in the open unit disk E

z:z 1

and Sbe the subclass of

Aconsisting of functions that are univalent inE.

Denote by P, the class of functions with positive real part, where functions in this class are of the form

   

1

1 ) (

n n nz

p z

(2)

et. al., 2018). Reade (1955) defined the class of close-to-starlike functions where functions in this class satisfy

 

 

z E

z z

f

     

, 0 Re

with

 

z belonging to S.

Reade (1955) obtained that f(z) is close-to-starlike if and only if the inequality,

 

 

 

 

    

 

 

d

re f

re f re

i i i

2

1

Re

holds for all12 and for all 0r1. The class of close-to-starlike functions is denoted by 

CS .

Srivastava and Attiya (2007) introduced a family of linear operatorJ,b:AA by the Hadamard product of the Hurwitz-Lerch Zeta function with analytic functions as

  

f z G f

 

z J,b,b

where bC withb0,1,2,3,, μC, zEand G,bA isgiven by

     

  

 

2 ,

1 ; , ) 1 (

n

n n b

z a b n

b z

b z b b

G

  

  

Srivastava et al. (2013), then introduced a subclass of close-to-starlike functions using Srivastava-Attiya operator denoted by

CS

s,b where they gave the following definition.

Definition 1.1 A function f is said to belong to the class

CS

s,b if and only if, there exists a function

g

S

 such that

  

 

0 , .

Re , z E

z g

z f

Jsb

   

 

In the special case whens0, the class

CS

s,bcan be reduced to the class CS, studied

earlier by Reade (1955).

This paper will define a new class of close-to-starlike functions using the operator defined by Carlson and Shaffer (1984), where the Carlson-Shaffer linear operator

A A : ) , ( 

L is given by

) ( ) ; , ( ) ( ) ,

(  f z    zf z L

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 

 

 

 

, 0, 1, 2, )

; , (

0 1

1 1 0

   

 

 

  

 

   

 

n

n n

n n

n n

n

z z

z z

The function,

(

,

;z) is known as the incomplete beta function. The term

(

)

k is the Pochhammer symbol that can be expanded in Gamma functions as

 

 

  

  

 

 

   

. , 2 , 1

1 1

0 1 : )

(  k k N 

k k

k

k

 

Thus, Carlson-Shaffer linear operator can be written as,

 

 

,

1

1a z E

n n n

n

 

 

z

z )f(z) , L(

2

n

(1.3)

We define our new class of functions as follows.

Definition 1.2 A function f is said to belong to the class of

CS

, if and only if there exists a function gSsuch that

Re

   

,

 

0, z E z

g z

f

   

 L 

(1.4)

In the special case, when 1 and 1, the class

CS

, reduces to the class CS, studied by Reade (1955).

The main objective of this paper is to find the coefficient inequalities and basic properties of the class

CS

,.

2. Coefficient bounds

Theorem 2.1 Let f in the form of (1.1) be in the class

CS

*,. Then,

 

 

, \



1

1 1

2 N

n

n a

n n

n

(2.1)

(4)

Let

    1 1 ) ( n n nz p z

p and

    1 ) ( n n nz b z z

g (2.3)

Then, by substituting (1.3) and (2.3) into (2.2), we have

, 1 1

2 1 1             

      b z p b b z z a z n n n k k n k n n n 2

n n-1

1 -n ) ( ) (   (2.4)

Comparing coefficient of

z

non both sides of (2.4) gives

.

2 1 1

      

n n k k n k n

n

b

b

p

a

2 n n-1

1 -n

)

(

)

(

(2.5) Also using the fact that



1

,

and

,

2

N

N

\

n

b

n

n

p

n n

equation (2.5) becomes



. n n k n a n k

n 2 1

1

1

2 N\

  

  1 -n 1 -n ) ( ) (

So, we have that,



1

,

2 N\

n n

an 1 -n 1 -n ) ( ) (

which will complete the proof of Theorem 2.1.

In its specific cases when

1 and

1, we obtain



1

,

2

N

\

n

n

a

n

which is the result of Reade (1955).

3. Growth and distortion theorem

Using the coefficient bound we now derive the other properties for the class

CS

*,. Firstly we find the growth theorem for functions in the class

CS

*,.

Theorem 3.1 Let

f

CS

*,. Then,

 

 

 

 

 

, z .

2 1 1 2 2 2 1 1 2 2 r E z n r r z f n r r n n n n n

n     

       

Proof Let

f

CS

*,. By taking absolute values on both sides of (1.1), we have

 

2 n n n

z

a

z

)

z

(

f

Hence, by using triangular inequalities, we have,

r

z

a

z

)

z

(

f

z

a

z

n n n n n

n

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 

2

2 n

n n n

n

n

r

f

(

z

)

r

a

r

a

r

. (3.1)

By substituting (2.1) into (3.1), we have

 

 

 

 

   

 

2 1

1 2 2

2 1

1 2 2

n n

n

n n

n

f

(

z

)

r

r

n

n

r

r

.

Thus this completes the proof of Theorem 3.1.

We next derive the distortion theorem for functions in the class

CS

,. Theorem 3.2 Let

f

CS

,. Then,

 

 

( ) 1

 

 

, z .

1

2 1

1 3

2 1

1 3

r E

z n

r z

f n

r

n n

n

n n

n      

   

  

Proof Let

f

CS

,. For distortion theorem, we differentiate (1.1) to obtain

 

1 2

1

n

n n

z

na

z

f

By taking absolute values on both sides, we have

1 2

1

)

(

n

n n

z

na

z

f

Hence, by using triangular inequalities, we have,

r

z

na

)

z

(

f

z

na

n

n n n

n

n

 

z

:

1

1

2

1 2

1

 

2

1 2

1 ( ) 1

1

n

n n n

n

nr f z na r

a

n (3.2)

By substituting (2.1) into (3.2), we have

 

 

 

 

   

 

2 1

1 3

2 1

1 3

1

1

n n

n

n n

n

f

(

z

)

r

n

n

r

.

Thus this completes the proof for Theorem 3.2.

4. Radius of convexity, starlikeness and close-to-convexity

Results on radius of convexity, starlikeness and close-to-convexity for the class CS*, will be obtained in this section.

A function fS is said to be convex of order (01) if

(6)

 

 

,



1

1 1

1

1 1

3  N\

            n n n z n n n     Proof

It is adequate to show that the values for 

        ) ( ) ( 1 z f z f z

liein a circle centered at w1 with

radius 1. We have

               

      1 1 1 1 ) ( ) ( 1 2 1 2 1 n n n n n n z a n z a n n z f z f z (4.2)

1

1

1

2 1 2 1            

      n n n n n

n z na z

a n

n

Finally, we get

1 1 2 1   

     n n n z a n n

In view of Theorem 2.1, we have

 

 

,



1 1 1 1 1 2 1 \ N        n n z n n n n n     (4.3)

Solving (4.3) for

z

we obtain

 

 

,



1.

1 1

1

1 1

3  N\

            n n n z n n n    

This completes the proof of Theorem 4.1.

A function fS is said to be starlike of order (01) if it satisfies

. ) ( ) (

Re 

       z f z f z (4.4)

Theorem 4.2 Let the functions in the form of (1.1) be in the class of CS*, . Then, f is starlike of order

if,

 

 

,



1.

1 1

1

1 1

2  N\

            n n n z n n n    

Proof We must show that,

       

      1 1 1 1 ) ( ) ( 2 1 2 1 n n n n n n z a z a n z f z f z (4.5)

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 

 

,



1 1

1 1

1 2 1

\ N

 

 

  

n n

z n

n n n

  

(4.6)

Solving (4.6) for

z

we obtain

 

 

,



1

1 1

1

1 1

2  N\

  

  

 

 

n

n n

z n

n n    

This completes the proof of Theorem 4.2.

A function fS is said to be close-to-convex of order (01) if

( )

.

Re fz

(4.7) Theorem 4.3 Let the functions in the form of (1.1) be in the class of

CS

*, . Then, f is close-to-convex of order

if,

 

 

,

n



.

n

z

n

n n

1

1

1

1

1 1

3

N

\

 

 

Proof We must show that

  

1 1

2

1

n

n n z

a n )

z (

f (4.8)

But in view of Theorem 2.1, the inequality (4.8) holds if

 

 

,



1

1

1

1

1 2 1

\

N

n

n

z

n

n n n

(4.9)

Solving (4.9) for

z

we obtain

 

 

,

n



.

n

z

n

n

n

1

1

1

1

1 1

3

N

\

 

 

This completes the proof of Theorem 4.3.

5. Conclusion

In this paper, a certain class of analytic functions in the complex plane is discussed. The class of analytic univalent functions is denoted by

S

.This paper is specifically focused on a class of close-to-starlike functions defined using Carlson-Shaffer operator. This class is denoted by

* , 

CS

.We find the coefficient bounds, growth and distortion theorems and radius properties

for the class defined.

References

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Hurwitz-Goodman, A. W. (1983). Univalent Functions, vols I & II,(Mariner publishing Company Inc., Tampa Florida, 1983).

Peter, O., Akinduko, O., Ishola, C., Afolabi, O., & Ganiyu, A. (2018). Series Solution Of Typhoid Fever Model Using Differential Transform Method. Malaysian Journal of Computing, 3(1), 67-80.

Rathi, S., Cik Soh, S., & Akbarally, A. (2018). Coefficient Bounds For A Certain Subclass Of Close-To-Convex Functions Associated With The Koebe Function. Malaysian Journal of Computing, 3(2), 172-177.

Reade, M. O. (1955). On close-to-convex univalent functions. Michigan Math. J., 3, 59-62.

References

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