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Irnat. J. Math. & Math. Si.

Vol. 6 No. 2 (1983) 335-340

335

ON THE RADIUS OF UNIVALENCE OF

CONVEX COMBINATIONS OF ANALYTIC FUNCTIONS

KHALIDA I. NOOR, FATIMA M. ALOBOUDI and NAEELA ALDIHAN

Mathematics Department

Science College of Education for Girls Malaz, Sitteen Road

Riyadh, SAUDI ARABIA

(Received July i0, 1982 and in revised form February 21, 1983)

ABSTRACT. We consider for a > 0, the convex combinations f(z) (l-a)F(z)

+ azF’(z),

where F belongs to different subclasses of univalent functions and find the radius for which f is in the same class.

KEY WORDS AND PHRASES. Univalent funtns, alpha-quasi-convex, stake, close-to- convex functio, nvex combinons.

1980 MATHEMATICS SUBJECT CLASSIFICATION CODES. Primary 30A32, Secondary 30A34.

1. INTRODUCTION.

Let S,

K,

S* and C denote the classes of analytic functions in the unit disc E

{z: zl

< i} which are respectively univalent, close-to-convex, starlike, and convex. In

[1,2],

a new subclass C* of univalent functions was introduced and studied.

A

function

f,

analytic in

E,

belongs to C* if and only if there exists a convex func- tion g such that for z g

E,

Re

(zf’(z))’

>

O. (i.i)

g’(z)

Tile functions in C* are called quasi-convex and C C* K S. It is shown

[2]

that f g C* if and only if

zf’

g K. Recently the functions called a-quasi-convex have been defined and their properties studied in

[3].

A function f, analytic in

E,

is said to be s-quasi-convex if and only if there exists a convex function g such that, for a

real and positive

f’(z)

Re{(l

a)

’-(z) +

a

(zf’ g’(z) (Z))’

> O, (1.2)

(2)

It has been shown

[3]

that F is s-quasl-convex if and only if f with

f(z) (i-

e)F(z) + zF’(z)

is close-to-convex.

(1.3)

All s-quasl-convex functions are close-to-convex.

2. MAIN RESULTS.

We shall now study the mapping properties of f:

f(z)

(i -)F(z)

+ zF’(z),

e >

0,

when F belongs to different subclasses of univalent functions.

THEOREM 2.1. Let F S* and > 0. The function

F(z)

(i-

)F(z) + zF’(z)

(2.1)

is starlike in

zl

<

ro,

where

This result is sharp.

ro

2

+ 2 +

i 2

(2.2)

PROOF. We can write (2.1) as

1 1

2 i

f(z) z (Z

F(z))’,

and from this it follows that

1 i

z -I -2

F(z) z z

0 Then

1 i

z.F’(z) {((i-

1 i---c

[z

---2

F(z)

)z z

0

1 1

i

{z z--2e

--1

{(i-

f(z)dz

+

z

0

f(z)dz

i i 1

z ---2

f(z)dz

+

f(z))/(z z

f(z)dz)}

0 i

f(z)}/{

z

f(z)dz} h(z),

(2.3)

(2.4)

where Re

h(z)

> 0, since F e S*.

From (2.4),

we have

I

Z

i

f(z)

-

i) 0 zC f(z)dz h(z) 0 zCi f(z)dz. (2.5)

Differentiating both sides of

(2.5),

we obtain

1 1 1

---2 ---i ---2

1

z(

z 1

zC

- I)

f(z)

+ f’

(z)

-

i) f(z)

=h’(z)

zz---2i f(z)dz+h(z)z---2e1 0

Thus

1

(z)

h(z),+

{h’(z)

zO

f(z) 0

i

f(z)dz}/{z

O

f(z)}.

f(Z)o

(3)

UNIVALENCE OF CONVEX COMBINATIONS OF ANALYTIC FUNCTIONS 337

Now,

using the well-known result

[4], lh’(z) -< {2Re h(z)}/(l

r

2), Izl

r, we have

z i

z-2f(z)dz

Re

zf’(z)> 2f(z)

Re

h(z){l-

’0 1

}"

(2.6) 1 r2

2 z f(z) From

(2.1)

and

(2.3),

we have

1 i

---i ---i

F(z))’

z

f(z

z(z

I i

z-2

f(z)dz (z

1F(z))

0

from which it follows that

1 1

l{z-if(z)/ Iz

0

z-2

i i

---i ---2

1 z

z{z

c

F’(z) +

-

i)

F(z)}

i

(z

c F(z)

zF’

(z) 1 1

Fz) +

i

-

i) i h(z)

+

1

(-

r i),

f(z)dz} >- Re{h(z) + -i)} >- (-i) +

1

+

r (2.7)

Using

(2.7),

we have from

(2.6)

2 Re

zf’(z)

> Re

h(z){l-

2 r

+

r

1

)}

2 1

+ (_

2)r

f(z) 1 r

c

i i i

le

4r-

- 2)r2)}/{(1

r)(

+ - 2r)}

Re hi

){(_.z._.

(2.8)

The right hand side of (2.8) is positive for r < r where r is given by (2.2). This

o o

result is sharp as can be seen by

1 i

f (z)

{C(z(

- - 2)z))}/(l

z)

o

(i- o)F (z)

+

OzF

’(z),

o o (2.9)

where

F

(z)

z

o (i- z)2 S*

RE}L%RK 2.1. Let f e C, then f, given by

(2.1),

is convex for

zl

< ro where ro

is given by

(2.2).

The proof follows on the same lines as in Theorem 2.1. See also

[5]

and

[6].

REMARK

2.2. In

[6],

Nikolaeva and Repnina treated the same problem, with a dif- ferent notation, for the convex and starlike functions of order

8.

Theorem 2.1 follows from their result when we take

’8

0 for 0 < < i. On the other

hand,

our proof of Theorem 2.1 is much simpler and the result holds for all > 0.

(4)

THEOREM 2.2. Let F e K and f(z) (i

e)F(z) + zF’(z),

>

O.

Then f is close-to-convex in

zl

< r0 r is given by (2 2). The function f0 in (2 9) shows

that this result is sharp.

PROOF. Since F E

K,

there exists a G e S* such that, for z E

E,

Re

zF’(z)

G(z) > 0.

Now let g(z) (i

)G(z) + zG’(z).

Then by Theorem 2.1 g is starlike for

Izl <r

O rO is defined by (2.2). Using the same technique of Theorem 2 1 we can easily show that Re

zf’(z

g(z) > 0 for

zl

< ro

REMARK 2.3. For a

1/2

this result has been proved in

[7].

As an easy consequence of

(1.3)

and Theorem 2.2, we have the following.

COROLLARY 2.1. Let F e K and f(z) (i

e)F(z) + azF’(z),

a > O. Then F is e- quasi-convex in

zl

< r This means that the radius of a-quasi-convexity for close-

O

to-convex functions is given by (2.2).

THEOREM 2.3. Let F g C* and a > 0. Let f(z) (i

a)F(z) + azF’(z).

Then f is in

C*,

for

Izl

<

ro,

r is given by

(2.2).

PROOF. Since F

C*,

there exists a G e C such that for z e

E,

Re

(zF’(z))’

G’ (z)

> 0, Now let g(z) (i )G(z)

+ zG’(z),

then g is convex in

zl

< rO We can write

1 1

2 i

f(z) (i a)F(z)

+ azF’(z)

z

F(z))’

and i i

2 1

g(z) (i

e)G(z) + ezG’(z)

z

G(z))’o

Thus

i i i i

2-E

z

E-I 2- z-

1

(zf’ (z) )’

g’(z) ((z(z F(z))’)’)’)/(z (( O(z))’)’)

Now

1 1

2 1

1 1

z

2F"

(z(z (z F(z))’)’)’ (z((-I)F(z) + zF’(z))’)’ zF’(z) + (z))

1 i i i i

2 i

o.

1 o

(Z Z

(2.10)

F’(z) +z F"(z)))’ (z (z zF’ (z)) ’) ’o

Let

zF’(z) H(z),

then from

(2.10),

we have

1 1 1 1

2 i 2 i

(zf’(z))’

(z e

z a

za

g’

(z) H(z))

’)’

/ (z G(z))

’)’

1 1

2 1

Since from Theorem 2.2, the function (l-)tt(z)

+ ztt’(z) It(z))’

be--.

longs to Kwith respect to a convex function g: g(z) (l-e)G(z)

+ ezG’(z)

in

(5)

UNIVALENCE OF CONVEX COMBINATIONS OF ANALYTIC FUNCTIONS 339

zl

< r0 so f is in C* for

zl

< r0 where r0 is given by

(2.2).

REMARK

2.4. For F e C* and

1/2,

Theorem 2.3 has been proved in

[1].

We now deal with a generalized form of (i.i) by taking g to be starlike and prove the following.

(zF’ (z))’

THEOREM 2.4. Let F be analytic in E and let for z e

E,

Re

G’(z)

>0, GeS*.

Let f(z) (l-)F(z)

+ zF’(z)

and g(z) (l-)G(z)

+ zG’ (z),

with e > 0.

Re

(.zf’ (z))’

g’(z)

> 0 for

Izl

<

rl,

where

Then

rI

3

+ 49

2

+

1- 2

For e

1/2,

the problem has been solved in

[8].

Thus

PROOF. From

(2.3),

we can write

I 1

1

i-

iz

---2C

F(z) z

0

f(z)dz

i i

1 i-- i

[z

2

j

z

zF

(.)

z

((1-)

0

i f(z)dz

+

za

f(z))

1 1

z za

f’

(z) dz) 0

(zF’ (z))’

G’(z)

1 1

I

fz

I

(zef ’(z) (-i)

z

f’(z)dz)

0

z 1 a i z 0

g’

(z)dz

h

(z),

(2.ii)

where Re h(z) > 0, z E.

From

(2.11),

we write

1 1 1

f,

i z --I

I

z --I

z (z)

(-i)

z

f’(z)dz

h(z) z

0 0

g’

(z)dz

Differentiating both sides, and simplifying, we obtain

(zf’ (z))’

g’(z)

=h(z)

+

i

h’ (z)(

z

J0

g’

(z) dz) 1

z

g’(z)

(2.12)

Using

lh’ (z)]

< 2Re h(z)

2-- (2.12)

gives

1 r

(6)

Re

(zf’ (z))_’

g’Cz)

> Re

h(z)[l

i

i r2 0

za

i

g’ (z)

dz) /(z g (z)dz) ]o (2.13)

Now

i i

I

z

E-

(zg (z))/(

z

g’

(z)dz) 0

(i/)G’(z) + zG"(z) G’(z)

i

(zG’ (z))’

(-i) + G’(z)

(2.14)

Since G e

S*,

so

(zG’

(z))’

G’(z)

l-4r+r2

2

(2.15)

From

(2.13), (2.14)

and

(2.15),

we obtain

Re

(zf’ (z))’

g’(z)

2 r(l- r

2)

>-

Re

h(z)[l

2 1

4r 1 2

1 r

-

2)r

1 6r-

(I 2)r

2 Re h(z) 2

1 4er (i 2)r

and this positive for

zl

<

rl,

where

r 1 1

3c

+ /9a

2

+

1 2a

ACKNOWLEDGEMENT. The authors are grateful for the referee’s helpful comments and suggestions on the earlier version of this paper. In particular, the reference to Nikolaeva and Repnina was kindly supplied by him.

REFERENCES

I. NOOR,

K.

INAYAT.

On a subclass of close-to-convex functions, Comm. Math. Univ.

St. Pauli

2__9 (1980),

25-28.

2.

NOOR,

K. INAYAT and

THOMAS,

D.K. On quasi-convex univalent functions, Inter. J.

Math. and Math. Sci. 3

(1980),

255-266.

3.

NOOR,

K. INAYAT and

ALOBOUDI, F.M.

Alpha-quasi-convex functions, to appear.

4.

LIBERA,

R.J. Some radius of convexity problems, Duke Math. J. 31

(1964),

143-158.

5.

CAMPBELL,

D.M. A survey of problems of the convex combination of univalent func- tions, Rockey Mount J. Math. 5

(1975),

475-492.

6.

NIKOLAEVA,

R.V. and

REPNINA,

L.G.

A

certain generalization of theorems due to Livingston, (Russian), Ukrain

Mat.

Z. 24

(1972),

268-273, MR45 # 5336.

7.

LIVINGSTON,

A.E. On the radius of univalence of certain analytic functions, Proc.

Amer.

Math. Soc. 17

(1966),

352-357.

8.

NOOR,

K INAYAT and

ALDIHAN,

N. A subclass of close-to-convex functions, to appear.

(7)

Mathematical Problems in Engineering

Special Issue on

Time-Dependent Billiards

Call for Papers

This subject has been extensively studied in the past years for one-, two-, and three-dimensional space. Additionally, such dynamical systems can exhibit a very important and still unexplained phenomenon, called as the Fermi acceleration phenomenon. Basically, the phenomenon of Fermi accelera- tion (FA) is a process in which a classical particle can acquire unbounded energy from collisions with a heavy moving wall.

This phenomenon was originally proposed by Enrico Fermi in 1949 as a possible explanation of the origin of the large energies of the cosmic particles. His original model was then modified and considered under different approaches and using many versions. Moreover, applications of FA have been of a large broad interest in many different fields of science including plasma physics, astrophysics, atomic physics, optics, and time-dependent billiard problems and they are useful for controlling chaos in Engineering and dynamical systems exhibiting chaos (both conservative and dissipative chaos).

We intend to publish in this special issue papers reporting research on time-dependent billiards. The topic includes both conservative and dissipative dynamics. Papers dis- cussing dynamical properties, statistical and mathematical results, stability investigation of the phase space structure, the phenomenon of Fermi acceleration, conditions for having suppression of Fermi acceleration, and computational and numerical methods for exploring these structures and applications are welcome.

To be acceptable for publication in the special issue of Mathematical Problems in Engineering, papers must make significant, original, and correct contributions to one or more of the topics above mentioned. Mathematical papers regarding the topics above are also welcome.

Authors should follow the Mathematical Problems in Engineering manuscript format described at

http://www .hindawi.com/journals/mpe/. Prospective authors should

submit an electronic copy of their complete manuscript through the journal Manuscript Tracking System at

http://

mts.hindawi.com/

according to the following timetable:

Manuscript Due December 1, 2008 First Round of Reviews March 1, 2009 Publication Date June 1, 2009

Guest Editors

Edson Denis Leonel,

Departamento de Estatística, Matemática Aplicada e Computação, Instituto de Geociências e Ciências Exatas, Universidade Estadual Paulista, Avenida 24A, 1515 Bela Vista, 13506-700 Rio Claro, SP, Brazil ; [email protected]

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