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C OMPOSITIO M ATHEMATICA

T ADAYUKI M ATSUZAWA S HUKICHI T ANNO

Estimates of the first eigenvalue of a big cup domain of a 2-sphere

Compositio Mathematica, tome 47, n

o

1 (1982), p. 95-100

<http://www.numdam.org/item?id=CM_1982__47_1_95_0>

© Foundation Compositio Mathematica, 1982, tous droits réservés.

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95

ESTIMATES OF THE FIRST EIGENVALUE OF A BIG CUP DOMAIN OF A 2-SPHERE

Tadayuki

Matsuzawa and Shukichi Tanno

@ 1982 Martinus Nijhoff Publishers - The Hague Printed in the Netherlands

Let

S2

=

(S2, go)

be the unit

2-sphere

in the Euclidean

3-space E3

and let

D(r)

denote a cup domain of

S2

which is the

geodesic

disk of

radius r centered at the south

pole Q. Let À1(r)

denote the first

eigenvalue

of the Dirichlet

problem

for

D(r).

For

’TT/2

r ’TT, we

have

2&#x3E;Bi(r)&#x3E;0.

However nice estimates of

À1(r)

seem to be un- known. For

example,

the value r for which

À1(r)

= 1 is related to the

study

of

stability

of minimal surfaces in

E4 (see [1],

p.

27),

and some estimate of r for which

À 1(r) &#x3E;

1 was

given

in

[1].

In this note we

give

estimates of

Ài(r)

for r which is near ’TT

(Theorem 1.1).

If we let r tend to ’TT, then

This agrees with a recent result

by

S. Ozawa

[5] (cf.

Remark ii in the section

2).

In the section

3,

as an

example,

we calculate our estimates for

r = 7T -

10-50;

Contrary

to 2-dimensional case, the first

eigenvalue

of a cup

domain of a unit

3-sphere S’

is

explicitly

calculatable

(see [4],

p.

154, [2],

p.

201).

We express our thanks to Mr. Muto for some comments.

1. The first

eigenvalue

of a cup domain

Let

(x,

y,

z)

be the canonical coordinates of

E3.

Then

S2 = {(x,

y,

z);

X2 + y2 + Z2 = 1}.

Put P =

(0, 0, 1)

and

Q

=

(0, 0, -1).

We denote the 0010-437X/82070095-06$00.20/0

(3)

96

Laplacian

on

S2 by

A. Then it is known that

satisfies

Af + 2f = 0

on

S2 - {P, QI

for any constant C.

f (z)

= 0 has

just

two solutions

for -1 z 1,

and solutions

depend

on C. Let

r =

r(x,

y,

z)

denote the distance function from

Q

on

S2.

Then

-

-W-e- fix- ro(6 ç-ro m-) and

consider the

corresponding

cup domaln

D(ro) = {(x,

y,

z)

E

S2; r(x,

y,

z):5 ro}.

Then we have some constant

C = C(ro)

such that the solutions y =

y(ro), (3

=

(3(ro)

of

fc(z)

= 0

satisfy

y

j8

= -cos ro.

Namely

C is determined

by (3 ;

Let z = a be the

point

where

fc(z)

takes its maximum. Then

and the maximum value is

equal

to

2/(1- a2).

We define a function F

on

D(ro) by

F is a

piecewise

smooth

C’-function

on

D(ro) vanishing

on the

boundary

of

D(ro).

Therefore the first

eigenvalue Ài(ro)

of D =

D(ro)

satisfies

Since the volume element of

D(ro)

is sin r dr A d0

(where

0 denotes

the rotation

parameter

around the

z-axis),

we get

(4)

Let D = D’ U

D",

where D’ denotes the part of D for z - a and D"

corresponds

to a

z (3.

Then

where the second

equality

follows from the fact that F vanishes on z =

J3

and the normal derivative of F vanishes on z = a. Theref ore we

get

THEOREM 1.1: Let

D(ro)

be a cup domain in

S2.

Then the

first eigenvalue À1(ro)

is estimated

by

where

/3, C,

a and A are determined

by

the

following :

PROOF: The first

inequality

of

(1.4)

f ollow s from a calculation

applying 0(t)

= sin t to Theorem 3 in

[3].

The second

inequality

of

(1.4)

is

(1.3). q.e.d.

REMARK i: Our

inequalities (1.4)

are most effective for ro= v. One merit of

(1.4)

is that it enables us to calculate

approximated

values of

À 1(ro),

ro =*= ’TT.

2. C alculation of A =

A(ro)

Here we calculate

(5)

98

We

put

u =

(1

+

z)/(l - z),

a =

(1

+

a)/(1- a)

and b =

(1

+

(3)/(1- 0).

Then,

dz = 2

dui(u

+

1)2

and

Continuing

calculations and

applying

we obtain the

following

PROPOSITION 2.1: For a =

(1

+

a)/(l - a )

and b =

(1

+

p)/(1 - 0),

The last term of

(2.1)

is estimated

by

the

following

PROPOSITION 2.2: For a &#x3E; 0 we have

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Next we

study

the behavior of

A(ro)

as r0 --&#x3E; 1r. We put 8 = 1- a and

p = 1 -

{3.

Then we get

etc.

By Propositions

2.1 and 2.2 we obtain

and hence for ro --- &#x3E; ir,

Therefore Theorem 1.3

implies

COROLLARY 2.3: Let

DE(P)

be an

E-neighborhood of

a

point

P in

S2.

Then the

first eigenvalue Àt,E of S2- DE(P) satisfies

PROOF: We put E=1T-ro. Then

1+cosro=E2/2+...,

and

Ài,e = À1(ro). Thus, (2.3)

follows from

(2.2). q.e.d.

REMARK ii. A result of S. Ozawa

[5]

is stated as

follows;

Let

(N, g)

be a compact 2-dimensional Riemannian manifold and let

DE(p)

be an

E-neighborhood

of a

point

p of N. Then the first

eigenvalue À1,E

of

(N, g) - DE(p)

satisfies

where

Vol(N, g)

denotes the volume of

(N, g).

His

proof depends

on

abstract

analysis,

and it is difficult to get the

geometric shape

of an

eigenfunction corresponding

to

AI,,,.

To get an

approximated shape

of

an

eigenf unction

the

following

observation is useful.

Any

2-dimen-

sional Reimannian manifold

(N, g)

is

locally

conformal to

(S2, go).

Let

U be a

neighborhood

of p in N and

let §

be a conformal map from U into

U* = ÇbU

in

S2.

We put P

= e(p).

If Eo is

sufficiently small,

for

any E Eo we have some

g = u(E)

such that the

boundary

of an

(7)

100

E-neighborhood DE(p)

of p in N is

mapped by 0

into

DE+u (P ) - DE_,(P)

in

S2.

The converse is also true. In the 2-dimensional case we

have another

special

property

that,

for

conformally

related metrics go and

g* = hgo (h : positive function)

the

Laplacians à

and A* cor-

responding

to go and

g* satisfy A*=(l/h)A/

for each function

f.

Therefore,

in an infinitesimal

domain,

h looks like a constant, and a function similar to F in the section 1 can be constructed in N.

3. An

example;

ro

= w - lo-50

As an

example

we calculate our estimate of

À1(ro)

for ro = 11’ -

10-o.

Estimate in the introduction

corresponds

to

REFERENCES

[1] J. L. BARBOSA and M. DO CARMO: Stability of minimal surfaces and eigenvalues of

the Laplacian. Math. Zeit. 173 (1980) 13-28.

[2] I. CHAVEL and E. A. FELDMAN: Spectra of domains in compact manifolds. Journ.

Funct. Anal. 30 (1978) 198-222.

[3] A. DEBIARD, B. GAVEAU et E. MAZET: Temps de sortie des boules normales et minoration local de 03BB1. Compt. Rend. Acad. Sci. Paris 278 (1974) 795-798.

[4] S. FRIEDLAND and W. K. HAYMAN: Eigenvalue inequalities for the Dirichlet problem on spheres and the growth of subharmonic functions. Comm. Math. Helv.

51 (1976) 133-161.

[5] S. OZAWA: The first eigenvalue of the Laplacian of two-dimensional Reimannian manifold (preprint; Department of Mathematics, Tokyo University, Japan).

(Oblatum 9-11-1981 &#x26; 29-VI-1981) Department of Mathematics Tokyo Institute of Technology Ohokayama, Meguro, Tokyo, Japan

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