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Annales Academie Scientiarum Fennice Series A. f. Mathematica

Volumen 12, 1987, 261-267

ON THE MAPPING WITH COMPLEX DILATATION

keio

EDGAR REICH

Abstract,

By

considering

the

explicit

form of the

quasiconformal mapping

Fxk)

of the complex plane with complex dilatation keiq

itis

possible

to

determine a sharp version

for

a variational lemma

for

extremal quasiconformal mappings

of

the

unit

disk. Additionally, we are led

to

an explicit elementary solution

of

a geo- metric extremal problem involving mappings

of

conic sections, which,

in

the case of ellipses, is equivalent to Teichmtiller's shift theorem, and, in the case of parabolas, reduces to a known example of non-unique extremality'

1. The mapping

ft(z)

Letkbe

a constånt,

-l<k<l.

Suppose

f (z)

is

a

qc (quasiconformal) map- ping of the regron O of the complex plane C satisfying the Beltrami equation

(1.1) x1(z):

* : OrnO: llsio

(z

:

rei\.

The complex dilatation

xlQ)

of (1.1) is of "Teichmtiller" form,

x1(z):

tiE6)1Ek)1, with

(r.2) Et4: I.

It

@(z) is a local determination of the integral

o@:*l'1@az=fr,

then

:

s@)

: o()+k6@ :

l/7

+kE

is a local solution of (1.1). The general qc solution,

w:f (z\,

of (1.1) in a particular region O therefore has

the

form A(SQ)), where zl(Q

is

analytic when (6rangeg, and zl is chosen so that

l(s|))

is single-valued homeomorphic

in

O.

In

particular, doi:10.5186/aasfm.1987.1231

(2)

262 EpcaR RrrcH

choosing

A(O:fu,

rz and denotine

^(Sk))by

FeQ), we obtain

(1.3) w: F*(z):fVu{r*2klzl+kzz).

It

is easily verified that F1,@) is one-to-one and maps

c

onto itself. Therefore, up to a linear transformation of the

v

plane, Fr(z) is the unique qc map of

c

with complex dilatation (1.1). For the real and imaginary parts,

w:u*iu,

of the mapping (1.3) we have

(1.4) ": lElQ+k)x+z*Wl,

and

(1.5)

o

: !.

Wenote

that FooEo:{", with c:(a*b)l1*ab).

lnparticular,

(1.6) .fi:'(r) : F-*(w):

i7@-2klwl+kz4.

2. Extremal qc mappings of the disk and the class ,4/

Let

o

be a proper subregion of the plane, and

let e: ea

denote the class

of

qc mappings

of

O. For

feQ, let

&,

: .ssup{lxr(z)l:

zcQ}, and,

for g(Q, let

Qlsl:

{.feQ:

flas =

glaal.

The basic extremal problem is to determine

(2.1) k*[g]:

inf

lk1: feQlsll

and corresponding extremal mapping(s)

f.eQlql.

Ahlfors'

[]

class .,1t

@)

which plays a basic role

in

the variational approach

p,

3l to the problem (2.1) is defined as follows. First,

let o(e)

denote the class

of

functions 9(z) holomorphic

in

O and belonging

to gt(Q):

llvll= [!rEQ)dxdy=*.

Then,

Jr(a): {nee*

rJy.

[[ o{z)E@)dxdy :0

for

all ,p<g@)\.

(3)

On the mapping with complex dilatation keto 263

The fundamental idea that

is

exploited

in

the variational approach

is

that

if

f€Qa,

and

xr€./r(O),

then

f (z)

is close

to

the identity on 0Q. Our purpose here is to derive a best possible quantitative version of this fact when Q is simply connected.

To this end,let

(2.2) xQ): sup{k*ffi: feQa,xf,ff(Q), kr* t},

0

<, <

1.

We observe that

if z*2

is a conformal map between O and O, then the rules E@)dzz

= O(4d22, "@*: r@*,

establish a correspondence between ,rf

@)

and -,{ (fr), which leaves

1(l)

unchanged.

Thus X(r) depends only on the value

of

/, not on the choice

of

O. Our result is as

follows.l

Theorem

2.1. Suppose

Q

is simply connected. Then

xQ): t2+o(ts), cts t *

o,

Proof.

In

view

of

the observation regarding invariance, we can assume that

o

is the unit

disk

11:{lzl<.1}.

An upper bound

for

yQ) is obtained using the following known inequality[4]:

(2.3) ,o*!il,. r-k*v1 = : ,kj==+I. r-k| '"

where

^I:

suP

lltt,%@E@ffi\'r'*r'r'

lleil

= 1)'

Since,

xr€tf (U\,

I I,.r*ffi : I I,

xrlxll,cP

##F

Therefore,

I€lårl[-k|).

Hence, by (2.3),

k*

tfl = &i

+

killt

+ k])

=

k', +

*i.

We therefore conclude [5] that

Q.4)

xG)

= tz+ts.

Consider, now, the mapping

F(z):

F,(z)'

wlrcre F,(z) as given by (1.2),

is

restricted

to llzl=l).

On 0U, F(z) agrees with the affine

maPPing

fr(z) : #e*rt+fz),

tA very closely related result is obtained by Lehto in [3J.

(4)

264 E»c.m Rnrcrr

which has complex dilatation

Since the affine mapping that

On the other hand, since

for

every function

Ek)

(2.5)

%to(z)

- t?.

of a region of finite area is extremal in its class,

it

follows

k*lFl:kfo:

t2.

0=t'<1, , have

d

f oe År

(U).

Consequently,

fi"

e" E ?''u) do

-

o,

holomorphic

in

(J, we

xQ)

=

t2.

3. Mapping of conic sections

By a conic section rve shall understand a region bounded by a circle, ellipse, parabola,

or

by a single branch

of

a hyperbola,

or

an angular region bounded by two rays.

Theorem

3:.1.

w:

F*(z) ffiaps euery conic section with focus at the origin onto a conic sectionwithfocus at the origin.

If

the conic section

Q

is a disk, ellipse, or para- bola, then

F{z)

is the unique extremal

qc

mapping among the class

of

mappings

g(z)

that satisfy

glao

:

Fnlan, g(0)

:

0.

(3.1)

Proof.

Let f :0Q.

We can assume that the major axis

of

the conic section lies on the

x

axis.

l-

satisfies an equation

(3.2) lzl

:

Ax

* p, (, - .r+

iy€T),

where.?,, is real and

p=Q. If -1=i.=1,

then

l-

is an ellipse with eccentricity

p'l andfociatthepoints z:0

and

z:2pil\-),'); if ).:*1,

and

p>0, then,l'is

a parabola;

if ),2-1,

then .l- is a branch of a hyperbola or the union of two rays.

Substituting (3.2) into (1.3), we flnd that

F{z)

is the restriction to

I

of the following affine mapping

(3.3)

1at:

A(z): #Kt+kl)z+(k+)")kz+2kpl.

Solving (3.3) for z in terms of w,

(3.4) z: A-L(w): r+#*Kt+H.)w-(k+),)kfr-2kp1.

:

When we substitute (3.4) into (1.6), we obtain

(5)

On the mapping with complex dilatation keto 26s

from which rve see that F1(O) is a conic section

and rl:0

a focus. Since

l(z)

is

a homeomorphism,

it

is clear that

if

i" is a circle or an ellipse, then its image is also

a circle or an ellipse, etc.

As regards the assertion of the theorem pertaining to the extremality

of

Fy(z), subject

to

the side conditions (3.1), one needs

to

make use

of

the fact,

(I.2), that

fr(z)

is a Teichmiiller mapping of

O\{0}, with

<p721:l/2. Since l/e is holomorphic

in O\{0},

unique extremality

of

Fp@), given the boundaryvalueson

å[O\{0}],

follows from classical facts [8J, providing (3.6)

//,..,,, lå

dx dv < oo.

x"t@): +:

Condition (3.6) is satisfied when O is bounded, i.e., a circle or ellipse. For the case when O is a parabolic region, the integral (3.6) is infinite, and not even extremality alone,

with or

without uniqueness,

is

a-priori clear. However, the fact

that a

qc

mapping of a parabolic region

with

complex dilatation (1.1)

is

uniquely extremal for its boundary values on the parabola and the focus was established by the author previously

[fl,

using a more refined analysis.

We note that the affine mapping A(z) of (3.3) has (k +

))k

l+kA

In particular,

)":tl, O=k<l

implies

ke:k.

This reflects the previously known

factl6, T

that F1,Q) and

A(z)

are both extremal mappings of parabolic regions with

focus

at z:0,

gioen the boundary aalues

of A(z)

on the parabola alone.

4. Shift mappings

Theorem

4.1.

Let E

be the Jordan region bounded by an ellipse

of

eccentricity

r,

whosefoci are

at 4

and 22. There is auniquely extremal qc tnap

h of E

onto

itself, keeping all points

of

0E fixed, and mapptng

zr

onto

zr.

The extremal dilation

k*

has the ualue

k*:kn:r. If 4:0,

and

z,

is on the negatioe real. axis, then

(4,1) h(z): t5«r*rrlzl+r2z)+zz.

Proof.

lf

the

foci

are

at z:Zptl(l-r2)

and

at z:0,

the equation

of åEis

lzl: -rx+p, (z: x*iy€08),

with p>0.

Consider now the image

of

.E under the mapping

w:F*(z\,

where

we set

k:r.

By (3.5),

with )t:-r, lc:r,

the equation of E,(åE) is

lwl: ru+p, (r: u+iu(\@E))t.

(6)

266 Eocan Rrrcn

4(.8)

is an ellipse with foci

at w:0

and

at w:2prl(l-22).

From (3.3),

it

is,

in

fact, clear that F"(08) is obtained from ä,8 by a pointwise translation

to

the right by a distance

2prl(l-rz).

Thus, h(z),as defined by (4.1), has the property that

it

keeps

all

points

of

åE fixed. The unique extremality property is a consequence

of

Theorem 3.1.

The above considerations are useful

in

clarifying Teichmiiller's construction of an extremal qc mapping of the disk onto itself which keeps all points of the cir- cumference fixed and shifts the origin

to a

specified

point.

Suppose

z:G(0

is

a conformal map

of

a region

A

onto the elliptical region .E

of

Theorem 4.1, with the foci located

at z:0, Z:zz<0.

Say,

G((6):0.

Then the mapping

(0,

defl- ned by

T(O

:

G-LohoG(o

all boundary prime ends fixed, while shifting (o

to

the

x1,(z)

- rzllzl,

z€.8,

it

fotlows that

f«)

is a Teichmiiller mapping with complex dilatation maps

fr

onto itself, keeping

point

G-tQr).

Since

(4.2) where (4,3)

The mapping

f(0

identity on Ofr and

xr0) _

ffi

%h(G(())

: rE l0JllE(ol,

EQ-lG

(Ol',lG(().

is uniquely extremal within the class of mappings which are the which shift (o

to T((i,

since

E«)

is holomorphicin

4\{(o},

and

//r.'.,

,orlQ0)ldoe

: { {r\ro}

#<oo'

References

[1] Anrrons, L. V.: Some remarks on Teichmiiller's space of Riemann surfaces, - Ann, of Math.

74, 1961, t7t-191.

[2] Krusmlr, S. L.: Extremal quasiconformal mappings. - Sibirsk. Malh. Zh, lO, 1969, 573-583 (Russian)

:

Siberian Math. J. 10, 1969,411-418.

[3] Lurro, O. : Application of singular integrals to extremal problems of Riemann surfaces. - Komp- leksnii analiz i ego prilozheniya (volume in honor of I. N. Vekua), "Nauka", Moscow, 1978,336-341.

[4] Rrrcn, E., and K, SrnnsrL: Extremal quasiconformal mappings with given boundary values. - Contributions to analysis, a collection of papers dedicated to Lipman Bers. Academic Press, New York-London, 1974, 37 5-391,

[5] Rucs, E.: On the decomposition of a class of ptane quasiconformal mappings. - Comment.

Math. Helv. 53, 1978, 15-27.

(7)

On the mapping with complex dilatation keta 267

[6] Rucn, E.: Nonuniqueness of Teichmiiller extremal mappings. - Proc. Amer. Math' Soc' 88' 1983, 513-516.

[7] Rrrcn, E.: On the structure of the family of extremal quasiconformal mappings of parabolic regions. - Complex Variables Theory Appl. 5, 1986, 289-300'

[8] SrxrsB1,

K.:

Zur Frage der Eindeutigkeit extremaler quasikonformer Abbildungen des Ein- heitskreises If. - Comment. Math. Helv. 39, 1964'77-89'

[9] Tucurratilr-rx, O,: Ein Verschiebungssatz der quasikonformen Abbildung.-Deutsche Math.

7,1944,336-343.

University of Minnesota School of Mathematics Minneapolis,

MN

55455

USA

Received 14 January 1987

ETH-Zentrum

Forschungsinstitut

fiir

Mathematik CH-8092 Zurich

Switzerland

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