• Aucun résultat trouvé

in lrl=l

N/A
N/A
Protected

Academic year: 2022

Partager "in lrl=l"

Copied!
2
0
0

Texte intégral

(1)

Annales Academire Scientiarum Fennicre Series A. I. Mathematica

Volumen 8, 1983 , 369-370

SOLUTIOI\S OF PROtsLEMS OF MILLER AND RUBEL

SAKARI TOPPILA

1. Introrluction and results.

Let w be

analytic

in lrl=l with w(0):0'

In

Problem 5.61 of [2] S. Miller states that

if n:l or n:2

and

(1.1) lw(z)+zw'(z)*...*znw@)(z)l=t for lrl=1,

then lw(z) | =

I for lzl-.1,

and he asks whether the same holds for all,

n:1,

2, 3, .. . .

We shall give an affirmative answer to this question'

Theorem

1.

Let w

be as aboae, satisfying

(l.t)for

some

n>3'

Then

lw(z)l''

71180

in lrl=1.

The following problem [1, Problem 2'54]is proposed by

L. A.

Rubel'

Problem A. Let E

be

a

closed set

in c with

the following properties:

(l)

there exists

a

transcendental entire function

f(z)

that

is

bounded

on E;

and

Q)

there exists

a

transcendmtal entire

function g(z)

that

is

bounded away from O on the complement oJ'

E.

For each such

E,

must there exist one ttanscendental entire function that is simultqneously bounded

on E

and bounded away

from O

on

the complement

of

E?

We shall give the following answer

to

this question.

Theorem 2. Let E

be the union

of

the positioe resl axis and the closed discs

lz-eak1=1,

k:1,2,

...

.

Then there exist transcendental entire functions

f1

and

f,

suchthat

fy

isboundedon

E

andthat

f,

isboundedawayJrom

0

onthecomplement

of E.

Howeaer,

if f

is any entire function which is bounded on

E

and bounded away

from 0

on the complement

of E,

then

f

is constant-

2. Proof of Theorem

1. Let n

and

w(z):

åo,*

be as

in

Theorem

l,

and let

s(z)

: w(z)* zw'(z)t...*

z'w@) 121

: )

boze'

Since

P=''

w@(z): ) onn(r-1)...(p- k+r1rn-u

p:L

doi:10.5186/aasfm.1983.0826

(2)

37A Saranr Toppna

and fr>3,

we

get br:2ar,

br-5o2,,

br-76os,

and

for p=4.

From (1.1) we deduce

that lbrl=t

for any

p,

and we get

-Z

loÅ

= U2*Us+Ut6+ lp-a =

6U80+

[ *-rdx :

7t180,

P:L p:a z

wnich implies

that

lw(z)l<.71l80

in lzl<1.

Theorem

I

is proved.

3.

Proof of

Theorem

2.

The function

fr(z):e-, is

bounded

on .E

and

fr(z) : II (l-

ze-4k) is bounded away

from 0

on the complement

of

.8.

Let us

suppose

that f is an

entire function which satisfies

lf(z)l=M

on

E and lfk)l=m (m>0)

on the complement

of

,E. From the continuity

of f it

follows

that lf(z)l>m

on the ring domain

e4k+L

<

lzl

-.

sax+t

for any

k.

Since eak+z€E, we deduce

that

lf(e4k+2)l=M, and applying Schottky's theorem repeatedly in the discs

lz

-

etk+z "i"1

-

eak+ 2 12,

we deduce that there exists

1(>0

depending only

on M

and

rz

such

that lf(z)l=K

for all

z

lying on the circle lzl:sak+a,

k:1,2,... .

This implies that

f

is a bounded

function and we deduce that

f

is constant. Theorem 2 is proved.

Refertnces

[1] ANonnsoN, J. M., K. F. Banrn, and D. A. BnaNNeN: Research problems in complex analysis. - Bull. London Math. Soc. 9, 1,977, 1,29-162.

[2] c.ltr@err,l, D. M., J. G. cruNre, and w. K. H,c,vM,{N: Research problems in complex analysis. - Aspects of contemporary complex analysis (Proceedings of an lnstructional Con- ference organized

by

the London Mathematical Society

at

the Univetsity of Durham, Durham 1979) edited by D. A. Brannan and J. G, Clunie, Academic press, London-New York-Toronto-Sydney-San Francisco, l9BO, 527-572.

University of Helsinki Department of Mathematics SF-00100 Helsinki 10

Finland

Received 25 }lfay 1983

Références

Documents relatifs

- Aspects of Contemporary Complex Analysis, Proceedings of an Instructional Conference organized by the London Mathe- matical Society at the University of Durham,

Though the women who originated from KEVI School, Birmingham, proceeded on the well-trod path to Newnham College, Cambridge, there were some women chemists at Mason College,

Les courbes de supersolubilité de leurs mélanges se rencontrent dans le mélange hypertectique contenant 74 0/0 de salol et dans lequel les deux substances se

vitesse des ions produits dans l’air, à la pression atmosphérique, par les rayons Rôntgen, et cela afin de savoir si la masse des ions dépend de la température....

solidus (et il y en a quatre dans le diagramme joint au mémoire) correspond à la cristallisation d’une série différente de solutions solides provenant du liquide,

tourne dans la même direction avec une vitesse angulaire deux fois plus grande. 11~ est à remarquer que la rotation du tube, tout en entraînant la rotation de l’image,

cope fut scellé dans un tube de verre renfermant un peu de vapeur d’eau saturée.. Dans ces conditions, les scintillations sont

En comparant les absorptions d’une solution colloïdale d’or dans l’eau avec les absorptions calculées de sphères et de molécules d’or diffusées dans l’eau, on