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ON CLOSE-TO-CONVEX FUNCTIONS OF COMPLEX ORDER

H.S.

AL-AMIRI

andTHOTAGE S. FERNANDO Department of Mathematics and Statistics

Bowling Green State University Bowling Green, OH 43403, USA (Received November 15, 1988)

ABSTRACT. The class

S*(b)

of starlike functions of complex order b was introduced and studied by M.K. Aouf and M.A. Nasr. The authors using the Ruscheweyh derivatives introduce the class K(b) of functions close-to-convex of complex order b, b 0 and its generalization, the classes

Kn(b)

where n is a nonnegatlve integer. Here

S*(b)

cK(b)

Ko(b).

Sharp coefficient bounds are determined for

Kn(b)

as well as several

sufficient conditions for functions to belong to

Kn(b).

The authors also obtain some distortion and covering theorems for

Kn(b)

and determine the radius of the largest

disk in which every f K (b) belongs to K (I). All results are sharp.

n n

KEY WORDS AND PHRASES. Starlike functions, close-to-convex functions of complex order, Ruscheweyh derivatives, Hadamard product.

1980 AMS SUBJECT CLASSIFICATION CODE. Primary 30C45.

I. INTRODUCTION.

Let A denote the class of functions f(z) analytic in the unit disk E {z:

zl <

I} having the power series

f(z) z + m=2

[. amZ

z e E. (1.1)

Aouf and Nasr [1] introduced the class

S*(b)

of starlike functions of order b, where b is a nonzero complex number, as follows:

S (b) f: f e A and Re +

f(z)

>

0, z e E}.

We define the class K(b) of close-to-convex functions of complex order b as follows: f K(b) if and only if f e A and

zf’

(z)

Re {I

+ g; I)}>

0, z

E,

(1.2)

for some starlike function g.

(2)

The classes

Rn,

n NO and where NO is the set of nonnegatlve integers, were introduced by Singh and Singh

[2],

f R if and only if f e A and

n

z(Dnf(z))

Re

> O,

z eE, (1.3)

Dnf(z)

where

Dnf(z)

f(z)

*

z

(1 z)n+l’ (1.4)

and (*) stands for the Hadamard product of power series, i.e., if

zn n

f(z) 0

.

an g(z) 0

.

bnzn then f(z)* g(z) 0 a bnnz

The operator Dn is referred to in Ai-Amiri [3] as the Ruscheweyh derivative of order n. Note that R

0 is the familiar class of starlike functions, S*. More, it is known [2] that

Rn+ 1CRn,

n

NO,

and consequently Rn consists of functions starlike in E.

Let

Kn(b)

n E

NO,

b is a nonzero complex number, denote the class of functions f g A satisfying

for some g Rn Here

K0(b)

K(b).

Many authors have studied various classes of univalent and multivalent functions using the Ruscheweyh derivatives D

n,

n N

O In particular one can look at the work of Ruscheweyh [4].

Section 2 determines coefficient estimates of functions in

Kn(b,

n e NO In

section 3, we obtain some distortion and covering theorems for

Kn(b)

and several

sufficient conditions for functions to be in

Kn(b).

The radius of close-to-convexlty for the class of close-to-convex of complex order b is also determined in section 3.

2. COEFFICIENT ESTIMATES.

In this section, sharp estimates for the coefficients of functions in

Kn(b)

are

determined in Theorem 2.1. First, we need the following lemmas.

LEMMA 2.1. For n

NO,

let

(Dnf(z)),

+ (2b- 1)z

3 (2.1)

(1 z) Then f E K (b).

n

PROOF. Let g A be defined so that

Dng(z)

z

(1 z)2

(3)

The definition of Rn implies g e R A brief computation gives n

[ z(Dnf(z))’ I]

+ z

+

Dng(z) ,

z z e E.

This proves that f K (b).

n

REMARK 2.I. The function f as defined in (2. has the power series representation in E

f(z) --z +mffi

.

2 n!(n +

<M-

m

I)!

1)! [(m 1)b + l]z

m.

(2.3)

.

m

NO

LEMMA 2.2. Let g(z) z + c z E R where n

m n

m--2 Then c 4 n! m!

m (n+m-

PROOF. A brief computation gives

Dn g(z) z + (n + m 1)! m

n:

(m 1)’ cz

mffi2 m

Since g E

Rn,

Dn g(z) E S Thus, using the well known coefficient estimates for starlike functions one gets

(n+m-1)!l

n! (m- 1)! cm m, m

>

2, and the proof is complete.

LEMMA 2.3. Let f(z) z + a zm If f K

(b),

n E

NO,

then

[ 12

Imam Cm 12

4 (n +(m m 1)!1)!

kffi2 (k I)

12[

PROOF. Let f(z) z + a z mffi2 m

be in

Kn(b).

Then (1.5) implies

[

z(Dn f(z))’

11

+ w(z)

+

Dn g(z)

l-

w(z) z e E, (2.5)

for some g e Rn and where w e A such that w(0) 0, w(z) and

Iw(z)l

for

(4)

z E. Let g(z) z + c z Then (2.5) and the Definition 1.4 imply m=2 m

w(z)

{n!

2bz +k=2

.

(n +(k k I)!I)!k=2

. [kak (n

(k- I)’.+ (2b+ k

-I)..! l)Ck]Z (kak k} Ck)zk

(2.6) Using Clunle’s method, that is to examine the bracketed quantity of the left-hand side in (2.6) and keep only those terms that involve zk for k m- for some fixed m, moving the other terms to the right side, one obtains

m-1

l[n!2bz

+

Lr

(n + k- I)’.

kffi2 (k l)!

[’kak

+ (2b

I.c kz kl,

m

.

(n + k I)’

Ck)Z

k

k=2 (k-l)’

(kak-

+ kffim+l

Akzk"

Let

m-1

l[n!2bz

+

Lr

(n +k I)!

k=2 (k 1)!

[kak

+ (2b

-l)Ck]Z k}

m (n + k I)’

zk k

k=2 (k I)

(kak Ck

+ k=m+l

- AkZ

(2.7)

Let z ret8 0

<

r

<

1. Computing

f

(z) (z) dz for both expressions of in (2.7) and using

Iw(z)l <

we get 0

.

(n + k- I)! 2

r2k

k=2 (k-l)

[kak Ck 12

ml [

(n + k-

1)’12

< n!2 41b12r2

+

kffi2 (k- 1)!

Ika

k+ (2b

1)ckl

2

r2k.

Upon letting r

1-and

after some easy computations we obtain

mam

Cm

2

k=2 (k- 1)!

In particular, when m 2 we have

(5)

The proof of the lemma is complete.

THEOREM 2.1. Let f(z) z +

[

a zm If f e K (b) where n e

NO

m=2 m n

then

n! (m- I)’

la

m < (n / m- 1)! [(m

1),b,

+ 1].

This result is sharp. An etremal function is given by (2.3).

m (b) Let the associate function of f, PROOF. Let f(z) z +

[

a z be in Kn

mffi2 m

g(z) z +

I cmzm"

We claim that for m ) 2 and n e

NO,

m=2

m (n + m- I)

2lb[

+

[.

(n + k- I)’

k= 2 n! (k-l)!

-Ck

(2.9)

We use the second principle of finite induction on m to prove (2.9).

n! 2(b)

is true as shown in (2.8) Now For m 2,

12a

2

-c21

(

<n

+ I),

21bl

(n + I)

assume (2.9) is true for all m (p. Taking m p + in

(2.4),

we get

I(P

+

l)ap+ Cp+ I12

Now using (2.9) since k p, the above yields n!

p!

!

l(p+l)ap+ Cp+ll

2

,

4

(n + p)

1512

P (n + k- I)!

k=2

(n +n!(-1)’

-

I)!

.C.

(n +n! (k- I)k- 1)

iCkl2

=2 kffi2

4

2 n! p!| 2

(n+p)!

J Ibl

I+2 kffi2 (n+k- I)!

+ 2 (n +k i)!

[

k-I

]

--2 "! (k- )!

I%1 I

(" +

-

P (n +k 1) 2

+ n’

<k-

),

,ck

k-2

(6)

Applying the principle of mathematical induction on p, it is easily seen that the sum of the last two terms appearing in the bracketed expression in the right hand slde of the above is equal to

!2 n!(n

(k+ k I)!I)! Consequently

it follows that

This shows that (2.9) is valid for m p + I.

Hence,

by the second principle of finite induction, the claim is correct From Lemma 2.2 and 2.9 it follows that

I.

m

-%. <

(n + m I)!

II

.>2. (2.,0)

Finally from Lemma 2.2 and 2.10 we deduce that

Hence the proof of the Theorem 2.1 is complete

Putting n 0 in Theorem 2.1 we have the following corollary.

COROLLARY 2 If f(z) z + a is a close-to-convex function of complex

mffi2 m

order b, then

I%1 <- )lbl

+ I. This result Is sharp.

REMARK 2.2. For b 1, Corollary 2.1 is reduced to the well known coefficient bounds for the close-to-convex functions due to Reade [5].

Next we have two theorems that provide sufficient conditions for a function to be in

Kn(b).

THEOREM 2.2. Let f e A and n E N

O If any of the following conditions is satisfied in E, then f K (b).

n

Re

{1 +

[(Dn f(z))’

I]} > O,

Re

{I +

[(I -z)(Dn f(z))’

I]} >

0,

Re

{I +

[(l z2)(Dn f(z))’

I]} >

0, (iv) Re

{I +

[(I -z)2 (Dn f(z))’

1]} >

0.

(7)

PROOF. The proofs follow by choosing g as below:

(i) g(z) z,

n! (m 1)! m

(ii) g(z) z +

(n + m 1) z m2

(iii) g(z) z +

[

n! (2m 2)! 2m-1

m=2 (n + 2m 2)! z and

n! m! m

(iv) g() +

(n + m 1) respectively.

m2

HgORgN 2.3. Let f() + a For n e

N0’

each of the following m-2 m

conditions is sufficient for f to be in

Kn(b).

(i) (n / m 1)!

m=2 n! (m 1)! m

[am[ [b[.

(n + m I)! (n + m)(m + 1)

a

Ib[

(ii)

[

n! (m 1)’

Ima

m=2 m m m+l

(iii) 2(n +

1)la2[ +m-2 [ n!(n +(mm_-2) [(m- 1)am_l-

(n +

m)(nm(m + m_ -l)l)(m

+ 1)

am+1,l lbl,

where a

I,

(iv)

21(n

+

1)a2 al

+

[

(n + m- 2)! 2(n + m l)

m=2 n! (m 2)!

[(m 1)am_l

m- am

(n + m)(n + m 1)(m + 1)

am/l!, ,Ibl’

where a 1.

I)

PROOF. We prove the sufficiency of part (1) since the proofs of the remaining parts are slmilar to the proof of (1).

From (1) of Theorem 2.2, f c

Kn(b)

if f satisfies the condition

Re

{1 + [(Dnf(z)) 1]} >

0, z c E. (2.11)

Condition (2.11) would be satisfied if

[(Dnf(z))’

I]

<

2, z c Z (2.12)

is true. However upon substituting

(Dnf(z))

+

[

m(n +n’ (mm I)’I) a zm m-1

in (2.12) one needs only show

(8)

II [-

m(n +(m m

)!

I)!

m=^Z n. a z

<

2, z eE.

m (2.13)

Assuming (1) of this theorem we have

,,,(.+m- ):

m-

)’

l

m=

-

2 n, (m I)! a zm

-*I Ib

m=

.

2 m(n +n! (m-m l)t.

,a

m’ +

<

2.

Thus (2.13) is established and the proof of the sufficiency of part (i) is complete.

REMARK 2.3. For n 0 and b

I,

Theorems 2.2 and 2.3 are reduced to theorems of Ozakl [6].

3. DISTORTION THEOREMS.

The objective of this section is to obtain some distortion theorems for the class The radius of the largest disk E(r)

{z/Is < r},

0

<

r 4 such that if

Kn(b).

f e K (b) then f K (I) can be determined as a consequence of one of those results.

n n

THEOREM 3.1. Let f e K (b) n e N

O Then for

Izl

r

<

and

12b ,

n

1-i2b- II= i,D

n

,,

1+

12b- !It

(3. I)

3

.,. f.z..’ <-

3

(1 + r) (1 r)

This result is sharp. An extremal function f is given by (2.1).

PROOF. Let f K (b). Then (I.5) implies for some g e R

n n

z(Dn f(z))’ + (2b I) w(z)

w(z) z E E,

Dng(z)

where w eA and

lw(z) , Izl

in E. This gives for

Izl

-r

<

-[2b- l[.r

+ r

, iz(Dn

f(z))’

, + j2b-

vng(z)

r (3.2)

The definition of Rn implies Dn

g(z)

is a starlike function. Hence by the well known bounds on functions which are starlike in

E,

we get for

zl

r

<

r

ID

n

g(z)l <

r

(I + r)2 (I r)2

(3.3)

Using (3.2) together with (3.3) one can get (3.1) and the proof of the Theorem 3.1 is complete.

Taking (1) n 0, and (ll) n 0, b in Theorem 3.1, one can immediately obtain the followlng corollarles, respectlvely.

COROLLARY 3.I. If f is a close-to-convex function of complex order b where

COROLLARY 3.2. If f is a close-to-convex function then for

zl

r

<

I,

(9)

1 -r l+r (1 + r)3

f’(z)

<

"(1

r)3

For the proof of Theorem 3.2, we need the following well known result [7; p. 84]

concerning the class P of functions p(z) which are regular in E such that p(0) and Re p(z)

>

0, z e E.

LEMMA 3.1. Let p e P. Then for

Izl

r

<

I,

2

,p(z’ +r

2 (3 4)

2 2

-r -r

This result is sharp.

THEOREM 3.2. Let f e K

(b),

n N

O Then for some g e R and for

Izl

r

<

I,

n n

[z(D

n f(z))’ + (2b- 1)r2

2[b[r

(3.5)

2 2"

Dn g(z) r r

This result is sharp. An extremal function is given in (2.1).

PROOF. f K (b) implies that for some g e R

n n

[z(D

n f(z))’

+

Dn g(z)

p(z),

z e E,

where p e P. Hence (3.5) can be obtained by substituting p(z) in (3.4).

It is interesting to note that the result in Theorem 3.2 does not depend on the value of n. Also, it can be used to solve the problem concerning the radii of

Kn(b)

in

Kn(1).

THEOREM 3.3. Let n e N

O If f e Kn

(b),

then f e Kn(I) for

Izl < r’

where

r

This result is also sharp. An extremal function is given in (2.1).

PROOF. Let f K (b). Then according to Theorem 3.2 there is some g e R such

n n

z(Dn f(z))’

Dn g(z) at + (2b l)r

and radius

-r2 -r

lles in the closed disk with center

It can be shown that this disk lles in the 2

right half plane if r

< r’.

This completes the proof of Theorem 3.3.

REMARK 3.1. Taking n 0 in Theorem 3.3, one can see that,

r’

is the sharp radius of close-to-convexlty for close-to-convex functions of complex order b.

(10)

REFERENCES

I. AOUF, M.K. and NASR, M.A., Starlike Functions of Complex Order b, J. Natural Sci. Math.

25(1), (1985),

1-12.

2. SINGH, S. and SINGH, S., Integrals of Certain Univalent Functions, Proc. Amer.

Math. Soc. 77(3),

(1979),

336-340.

3.

AL-AMIRI,

R.S., On Ruscheweyh Derivatives, Annales Polanlc Math.,

38(I), (1980),

88-94.

4. RUSCHEWEYH, S., Convolutions in Geometric Function Theory, Les Presses De l’Unlversite De Montreal (1982)

5. READE, M.O., On Close-to-Convex Univalent Functions,

Mlchlan

Mah. J., 3,

(1955), 59-62.

6. OZAKI, S., On The Theory of Multlvalent Functions,

cl. Pep. Tokyo

Burnlka Paig.

A2

(1935),

167-188.

7. GOODMAN, A.W., Univalent Functions1, Marlnar Publishing Company Inc.

8. CLUNIE,

J.,

On Meromorphic Schllcht Functions, J. London Math. Soc. 34 (1952), 215-216.

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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

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

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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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Hindawi Publishing Corporation http://www.hindawi.com

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