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(1)

A NNALI DELLA

S CUOLA N ORMALE S UPERIORE DI P ISA Classe di Scienze

M ITSURU N AKAI L EO S ARIO

Manifolds with strong harmonic boundaries but without Green’s functions of clamped bodies

Annali della Scuola Normale Superiore di Pisa, Classe di Scienze 4

e

série, tome 3, n

o

4 (1976), p. 665-670

<http://www.numdam.org/item?id=ASNSP_1976_4_3_4_665_0>

© Scuola Normale Superiore, Pisa, 1976, tous droits réservés.

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Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques

http://www.numdam.org/

(2)

but without Green’s Functions of Clamped Bodies (*).

MITSURU NAKAI

(**) -

LEO SARIO

(***)

We are interested in

costructing,

on a

given

Riemannian manifold

M,

the biharmonic Green’s function

PM(X, y)

of the

clamped body,

characterized

by

on

M,

with

~~

the Dirac measure

at y,

and the « Dirichlet data

at the ideal

boundary

of M ». The function is the

analogue

of the Green’s

function of the

clamped plate, significant

in the

theory

of

elasticity.

The

construction of the function and the nature of

(2)

have been discussed in

Ralston-Sario

[6]

from the view

point

of a

priori

estimates and in Nakai- Sario

[2]-[4]

from the view

point

of kernel

potentials.

We denote

by

the class of

noncompact

Riemannian manifolds M which do not

carry PMe

Several

complete

characterizations of the class

0~

were obtained in Nakai-Sario

[5].

The natural

question

arises as to whether or not a harmonic

nondegeneracy

of the ideal

boundary

of M is sufficient to entail the existence of We denote

by OHx

the class of Riemannian manifolds M which carry no non- constant harmonic functions with the

property

X = P

(positive), B (bounded),

y

(*)

The work was

sponsored by

the U.S.

Army

Research Office, Grant DA-

ARO-31-124-73-G39. MOS Classification 31B30.

(**) Nagoya

Institute of

Technology.

(***) University

of California, Los

Angeles.

Pervenuto alla Redazione il 15 Dicembre 1975.

43 - .dnn,ati della Scuola Norm. Sup. di Pisa

(3)

666

D

(Dirichlet finite),

or BD

(B

and

D).

Let

0~

be the class of

parabolic

mani-

folds. The

following

strict inclusion relations are well known

(Schiffer-Sario-

Glasner

[8], Hada-Sario-Wang [1], and,

for a

complete reference,

Sario-

Nakai [7]) :

Thus the

strongest

harmonic

nondegeneracy

is and we ask ex-

plicitly :

does assure that The purpose of the

present

paper is to show that the answer is in the

negative, i. e. ,

and this relation holds for every dimension

N ~ 2

of the manifold. Since any

subregion

of the Euclidean

N-space

EN for

N&#x3E;5,

and any

subregion

of EN with an exterior

point

for

N = 2, 3, 4 carries @ (Nakai-Sario [4]),

a manifold in

(5)

will

be, by necessity,

somewhat intricate.

1. - Consider the sets

in the Euclidean space EN of dimension

N ~ 2 .

Denote

by

the double of ~N with

respect

to

i.e.,

the

topological

manifold u

defined in an obvious manner, y with the i

(i = 1, 2)

du-

plicates

of ~N.

In terms of the

polar

coordinates

(r, 0) = (r, 01,

...,

ON-’)

of

points

x =

(xl, ... , xN), [x [ = r,

in ~N the Euclidean metric

(line element) Idxl I

is

given by

We introduce the Riemannian metric

on

with cp and y strictly positive

C°° functions on

[1, 00)

such

that

(9)

defines a 000 metric on

2N by symmetry.

Denote

by

(4)

the manifold

~

with metric

(9).

We could

actually

allow ds to be any

smooth metric on

(10)

as

long

as it satisfies

(9)

on a

neighborhood

of each

«

point

at

infinity)} ði =1, 2 ), i. e. , duplicate

in

=1, 2 )

of the

point

at infinite ð of EN and hence of EN. The manifold

2§f

can also be viewed

as the double

of

the Riemannian

mani f oZd ~~ ~

=

(EN, ds)

with

respect

to TN.

2. - We consider the

following

two conditions on the

functions cp and "p:

The existence of functions

satisfying

these conditions is

obvious,

the choice

q~ (r )

=

r2

and

y(r)

=

r- ~N- s»(N-1&#x3E;

for

large

r

being

an

example.

The purpose of the

present

paper is to prove:

THEOREM. The

mani f otd (N ~ 2 )

carries nonconstant Dirichlet

finite

harmonic

functions, yet

does not admit the biharmonic Green’s

of

the

clamped body, i.e.,

if

and

only if

the

functions

g~

and y satisly

conditions

(11 )

and

(12).

We will prove, in Nos. 3 and 4

below,

two

propositions, A)

and

B),

from

which the above theorem will follow at once.

3. - Denote

by W = W(a) (0’&#x3E; 1)

the

region

in

~N,

and

by Wi =

i its

duplicates

in

(EN)

i

(i =1, 2 ) .

On each

W(a)o

the

Laplace-

Beltrami

operator

L1 = db

-E-

d for takes the form

with If

(11)

is

satisfied,

then

(5)

668

is a harmonic function on This means that the hacrmonic measure

1-

a) of 6

i with

respect

to

W(ai)

is

positive and, therefore,

with the class of those Riemannian manifolds M with

compact

or

noncompact distinguished

smooth boundaries y which carry no nonconstant

Dirichlet

finite harmonic functions with

boundary

values zero on y.

By

the two

region

criterion

(cf.,

e.g., Sario-Nakai

[7]), (16) implies

that

if

(11)

is assumed.

Suppose

now that

(11)

is not valid. The function

is also harmonic on

W(a),

but

(i =1, 2). Hence, and,

a

fortiori,

We have shown :

A)

The

manifold °HD il

and the

and

satisly (11).

4. - The surface element of TN considered in EN is d6 =

~,(o) dol ... doN-1,

with finite total measure

Therefore,

the surface element

of I x =

r &#x3E; a in

±~v

is and the

volume element of i in

11

is

Under

assumption (11),

the condition

(12)

is thus

equivalent

to

If we assume that

(12),

or

equivalently (18),

y does not

hold,

then

by

the

Ralston-Sario theorem

[6]

or

by

the Nakai-Sario theorem

[~ ],

we conclude

that

~~ ~ ~ 0~ .

°

(6)

Conversely

assume, under

assumption (11),

that

~~ ,~ ~ 0~ .

We wish to

deduce the

invalidity

of

(12),

or

equivalently,

of

(18).

The

proof

is

by

con-

tradiction.

Suppose

that

(12),

or

equivalently (18),

holds. Fix an

arbitrary

and then a such that Let

Then, by Nakai-Sario [2 ]- [5 ] ,

we have

The function h =

.HM( ~ , y) has,

for any fixed r &#x3E;, cr, the « Fourier

expansion »

where

(m = i,

...,

mn)

is a

complete

orthonormal

system

of

spherical

harmonics of

degree n ~ 1,

and thus U

(n = 1, 2,

... ; m

= 11

...,

mn)

is a

complete

orthonormal

system

in

L2(TN; dO). By

the Parseval

identity,

for every

oo).

Since

ho(r)

satisfies

dho = 0

and

hnm(r)

satisfies the

« P-harmonic

equation &#x3E;&#x3E;

we see that

ho

and

hnm

are all subharmonic on

W(a)i w W(G)2

and con-

sequently f (r)

is subharmonic on u

W(G)2. Therefore, f (r)

takes on

its maximum in

[a, oo)

at a or b.

By (19),

As a direct consequence of

(12),

we see that

(7)

670

In view of

(22)

and

(23),

we must have

lim inf,-+oo f (r)

=

0, i.e.,

there exists an

increasing divergent

sequence

~rn~

in such that

f(rn)

-~ 0

( n -~ oo ) .

Since

for every

n = 1, 2, ...,

we have

f(r)

=

0, i.e.,

This with and the maximum

principle yields

on

2§~~ . Again by

the maximum

principle, 2v( ~ , ~) c cH~( ~ , y)

on

U

1~(y)2?

with c = 00. Hence

However,

this is

impossible

in view of

(18)

and

(19).

Thus

w 0p implies

that

(12)

is not satisfied.

B)

Under

assumption (11),

the

manilold

E

0,0 i f

and

only if

the

f unctions

qJ and 1p

satisfy (12).

REFERENCES

[1]

D. HADA - L. SARIO - C. WANG,

N-manifolds carrying

bounded but no Dirichlet

finite

harmonic

functions, Nagoya

Math. J., 54

(1974),

pp. 1-6.

[2]

M. NAKAI - L. SARIO, Parabolic Riemannian

planes carrying

biharmonic Green’s

functions of

the

clamped plate,

J.

Analyse

Math. (to

appear).

[3]

M. NAKAI - L. SARIO, A strict inclusion related to biharmonic Green’s

functions of clamped

and

simply supported

bodies, Ann. Acad. Sci. Fenn. (to

appear).

[4]

M. NAKAI L. SARIO, Existence

of

biharmonic Green’s

functions

(to

appear).

[5]

M. NAKAI - L. SARIO, A nonexistence test

for

biharmonic Green’s

functions of clamped

bodies, Math. Scand. (to

appear).

[6]

J. RALSTON - L. SARIO, A relation between biharmonic Green’s

functions of simply supported

and

clamped

bodies,

Nagoya

Math. J.

(to appear).

[7]

L. SARIO - M. NAKAI,

Classification Theory of

Riemann

Surfaces,

Grundlehren vol. 164,

Springer-Verlag, Berlin-Heidelberg-New

York

(1970),

446 pp.

[8]

L. SARIO - M. SCHIFFER - M. GLASNER, The span and

principal functions

on Riemannian spaces, J.

Analyse

Math., 15 (1965), pp. 115-134.

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