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Internat. J. Math. & Math. Sci.

Vol. 24, No. 7 (2000) 433–435 S0161171200004634

© Hindawi Publishing Corp.

A SUBORDINATION THEOREM FOR SPIRALLIKE FUNCTIONS

SUKHJIT SINGH (Received 24 November 1999)

Abstract.We prove a subordination relation for a subclass of the class ofλ-spirallike functions.

Keywords and phrases. Convex function, spirallike function, subordinating factor sequence.

2000 Mathematics Subject Classification. Primary 30C45; Secondary 30C50.

1. Introduction. LetKdenote the usual class of convex functions. Denote bySp(λ),

−π/2< λ < π/2, the class of functionsf (z)=z+a2z2+···which are analytic inE and satisfy therein the condition

Re

ezf(z) f (z)

>0. (1.1)

Spacek [3] proved that members ofSp(λ), known asλspirallike functions, are univa- lent inE. In 1989, Silverman [2] proved that if

n=2

1+(n−1)secλan1

|λ|<π 2

, (1.2)

then the functionf (z)=z+ n=2anznbelongs toSp(λ). Let us denote byG(λ),the class of functionf (z)=z+ n=2anznwhose coefficients satisfy the condition (1.2).

Note that G(0)is a subclass of the class of starlike functions (with respect to the origin) (see Silverman [1]).

In this paper, we prove a subordination theorem for the classG(λ). To state and prove our main result we need the following definitions and lemma.

Definition1.1. Iff (z)= n=0anznandg(z)= n=0bnznare analytic in|z|< r, then their Hadamard product/convolution,fgis the function defined by the power series

(f∗g)(z)= n=0

anbnzn. (1.3)

The functionf∗gis also analytic in|z|< r.

Definition1.2. Letf be analytic inE, ganalytic and univalent inE andf (0)= g(0). Then by the symbolf (z)g(z)(fsubordinate tog) inE, we shall mean that f (E)g(E).

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434 SUKHJIT SINGH

Definition1.3. A sequence{bn}1 of complex numbers is said to be a subordi- nating factor sequence if wheneverf (z)= k=1akzk, a1=1 is regular, univalent and convex inE, we have

k=1

bkakzkf (z) inE. (1.4)

Lemma1.4. The sequence{bn}1 is a subordinating factor sequence if and only if Re

1+2

n=1

bnzn

>0, (zE). (1.5)

This lemma which gives a beautiful characterisation of a subordinating factor se- quence is due to Wilf [4].

2. Main theorem

Theorem2.1. LetfG(λ). Then 1+secλ

2(2+secλ)(f∗g)(z)g(z), (zE) (2.1) for every functiongin the classK.

In particular

Ref (z) > 2+secλ

(1+secλ), (zE). (2.2)

The constant(1+secλ)/2(2+secλ)cannot be replaced by any larger one.

Takingλ=0, we obtain the following corollary.

Corollary2.2. Iff (z)=z+a2z2+ ··· is regular inE and satisfies therein the condition

n=2

nan1, (2.3)

then for every functionginK, we have 1

3(fg)(z)g(z), (|z|<1). (2.4) In particular,Ref (z) >−3/2, zE. The constant1/3is best possible.

Proof of Theorem2.1. Let f (z)=z+ n=2anzn be any member of the class G(λ)and letg(z)=z+ n=2cnznbe any function in the classK. Then

1+secλ

2(2+secλ)(fg)(z)= 1+secλ 2(2+secλ)

z+

n=2

ancnzn

. (2.5)

Thus, by Definition 1.3, the assertion of our theorem will hold if the sequence (1+secλ)an

2(2+secλ)

n=1

(2.6) is a subordinating factor sequence, witha1=1. In view of the lemma, this will be the

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A SUBORDINATION THEOREM FOR SPIRALLIKE FUNCTIONS 435 case if and only if

Re

1+2 n=1

1+secλ 2(2+secλ)anzn

>0, (zE). (2.7) Now

Re

1+1+secλ 2+secλ

n=1

anzn

=Re

1+1+secλ

2+secλz+ 1 2+secλ

n=2

(1+secλ)anzn

>

11+secλ

2+secλr 1 2+secλ

n=2

1+(n1)secλanrn

(because 1+secλ1+(n1)secλfor alln2,|λ|< π/2)

>

11+secλ

2+secλr 1 2+secλr

(|z| =r )

>0.

(2.8)

Thus (2.7) holds true in E. This proves the first assertion. That Ref (z) > −(2+ secλ)/(1+secλ)forfG(λ)follows by takingg(z)=z/(1−z)in (2.1). To prove the sharpness of the constant(1+secλ)/2(2+secλ), we consider the functionf0defined byf0(z)=z−(1/(1+secλ))z2(|λ|< π/2), which is a member of the classG(λ). Thus from the relation (2.1) we obtain

1+secλ

2(2+secλ)f0(z) z

1−z. (2.9)

It can be easily verified that

|z|≤1minRe

1+secλ 2(2+secλ)f0(z)

= −1

2. (2.10)

This shows that the constant(1+secλ)/2(2+secλ)is best possible.

Acknowledgement. This paper was presented at the 62nd annual conference of the Indian Mathematical Society held at IIT, Kanpur from December 22–25, 1996.

The author is thankful to Prof. Ram Singh, Department of Mathematics, Punjabi University, Patiala, for his help and encouragement during this work.

References

[1] H. Silverman,Univalent functions with negative coefficients, Proc. Amer. Math. Soc.51 (1975), 109–116. MR 51#5910. Zbl 311.30007.

[2] , Sufficient conditions for spiral-likeness, Int. J. Math. Math. Sci.12(1989), no. 4, 641–644. MR 90k:30024. Zbl 688.30009.

[3] L. Spacek,Contribution à la theorie des fonctions univalents, Cas. Mat. Fys.62(1932), no. 2, 12–19 (Czech). Zbl 006.06403.

[4] H. S. Wilf,Subordinating factor sequences for convex maps of the unit circle, Proc. Amer.

Math. Soc.12(1961), 689–693. MR 23#A2519. Zbl 100.07201.

Sukhjit Singh: Department of Mathematics, Sant Longowal Institute of Engineering

& Technology, Longowal-148 106(Punjab), India

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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 athttp://

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]

Alexander Loskutov,Physics Faculty, Moscow State University, Vorob’evy Gory, Moscow 119992, Russia;

[email protected]

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

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