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A NNALES DE LA FACULTÉ DES SCIENCES DE T OULOUSE

O ULD A HMED -I ZID -B IH I SSELKOU

Critical boundary constants and Pohozaev identity

Annales de la faculté des sciences de Toulouse 6

e

série, tome 10, n

o

2 (2001), p. 347-359

<http://www.numdam.org/item?id=AFST_2001_6_10_2_347_0>

© Université Paul Sabatier, 2001, tous droits réservés.

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Toute utilisation commerciale ou impression systématique est constitu- tive d’une infraction pénale. Toute copie ou impression de ce fichier doit contenir la présente mention de copyright.

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

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- 347 -

Critical boundary constants

and Pohozaev identity (*)

OULD AHMED-IZID-BIH ISSELKOU (1)

E-mail: [email protected]

Annales de la Faculte des Sciences de Toulouse Vol. X, 2, 2001

pp. 347-359

a mes deux

filles

Kénizé et Maöna

RESUME. - La premiere partie de ce travail concerne le probleme,

On démontre qu’il existe une constante critique

~*=(n(n-2) 4)n-2 4,

telle

que le problème

(PE)

admet exactement deux solutions u~1 et u~2

(u~1 u~2)

si 0 E E*, une solution unique si E = E* et n’admet pas de solution si E > E* .Toutes ces solutions seront données explicitement. Il est démontré que quand E ~ 0,

Au cours de la seconde partie, on s’intéresse au probleme

ou Q est un domaine borne, regulier et etoile par rapport a l’origine, f

est continue et depend asymptotiquement de u "comme ua", 1 a et

a ~ n+2 n-2. Différents résultats d’existence de constante au bord critique e* pour le probleme

(Qe)

sont donnes.

ABSTRACT. - The first part of this work deals with the problem

( _ ;~±2

( * ) > Recu le 21 mai 2000, accepte le 29 janvier 2001

(1) Faculte des Sciences et Techniques, B.P. 5026 Nouakchott, Mauritanie and The Abdus Salam ICTP, Trieste, Italy.

(3)

n. - 2

We show that there exists a critical constant

E* - ~ n~ 4 2~ ) 4 ,

such

that the problem

(PE)

admits two solutions u~1 and u~2

(u~1 u~2)

if

0 E E*, only one solution if E = E* and no solution if E > E* .We give

all these solutions explicitly.We show that, when E --~ 0,

The second part is devoted to the following problem

where Q is a regular bounded domain which is starshaped about the origin, f is continuous and behaves like u‘~ in the second variable, 1 a and o; ~

’’~§-

We give different existence results for a boundary critical datum e* for

(Qe).

1. The Sobolev

Exponent

Growth

Let us consider the

problem

In

[9],

it is shown that there exists a critical

boundary

datum E* such that

V 0 E

E*, (PE)

admits -at least- one

C2-solution.

There is no solution when E > 6*. It is known that

(PO)

does not admit a nontrivial solution

(see [13]). According

to

[5],

every

regular

solution of

(PE)

is

spherically symmetric. Let uE (E

>

0),

be a solution of

(PE),

then

is a solution of

where

(4)

The maximum

principle implies

It is known

(see [11],[4]

and

[3])

that there exists a constant A* such that

(AB) admits just

two

C3 - spherically symmetric

solutions when 0 A

~ * , only

one solution for A = A* and no solution if A > A*. We

give

here the

value of A* and the

explicit

solutions for

every ~

A*. We show that when

~ -~

0,

the "small" solution tends to v = 0 the trivial solution of

(AO)

and

the

"big"

one tends to

H(x)

=

1,

x

7~

O.

PROPOSITION 1

Proo f.

For

let uE be a

regular (Pe)

solution. As in

[13],

let us

put

and use the

Divergence Theorem,

to

get

From the

identity

we infer that

(5)

Using again

the

Divergence Theorem,

we

get

where v denotes the unit outward normal to

~B1.

The Maximum

Principle implies

that

As Vf;

is

spherically symmetric

and vanishs on

~B1,

we

get

where l is a constant on

~B1. Using

the fact that x.v = 1 on

aBl,

we obtain

from (*1

This

equation

is

equivalent

to

where Bl is

the

Lebesgue

measure of the unit ball of Rn and

|S1|

=

is the surface measure of the unit

sphere.

We obtain the

following equation

in l =

When

this

equation

admits two

negative

solutions

(6)

When

equation (1)

admits a

unique negative

solution

and no real solution if

So it is clear that

The

proof

will be

complete,

if one shows that

there exists

just

two

regular

solutions of

(PE).

Let us recall that the

problem

admits the radial solutions

(see [12])

Let us

put

It is immediate to

verify

that

In

particular,

(7)

As the function

is continuous on with

we obtain two distinct solutions of

(PE),

when

and one solution when

which is

~i.

So the

proof

of

Proposition

1 is

complete.

Let us

study

the behavior of solutions when Let uEl and uE2 be the two solutions of

(PE),

with

and

such that

Let us

put

(8)

PROPOSITION 2

Proof.

Let us remark the

following

We

give

here a direct

proof, using

the

explicit knowledge

of

i E ~1, 2~.

As we have seen, for every 0 E

E*,

there exists a

unique

such that we have

We

finally get

It is immediate to

verify

that

and

Remark 1. -

According

to Theorem 1.1 in it

is,

in

general, false

that every

positive

solution u in

B1 of

Du + ~ca =

0,

is a restriction

of

a

positive

solution v

of

this

problem

in ~’~ .

(9)

2. Nonlinearities with Noncritical Growth 2.1. The Subcritical Behavior

We deal here with the

following problem

Let us suppose the

following

(i)

SZ is a bounded

regular

domain of

~n,

which is

starshaped

about

the

origin.

(ii) (’0 x ~+, ~J2+) ,

(iii)

there exist

positive

constants and a

positive

function a E

such that

lim

t)

=

a(x)

and

f(x, t)

=

o(t)

near t =

0, uniformly

in x E 03A9.

to.

PROPOSITION 3.2014 Under the

previous hypotheses

on SZ and

f , there

exists a

positive

constant

E* (SZ, f ),

such that

for every_0 E E* (SZ, f),

the

problem (QE) admits,

at

least,

one

solution u~ ~ C1,03B4 (03A9)

,

0 03B4

1. . There

is no bounded solution

of (QE) if

E >

E* (SZ, f ) .

Proof.

The

proof

is

nearly

the same as in

(Theorem

1 in

[9]).

The

only

difference is that the subsolutions and

supersolutions

are considered as

elements of n and the

inequalities

are in the sense of

duality

H-1(~) ~ Ho (~)~

°

Let us recall the main

steps

for this

proof.

1. We use the

hypothesis (iii)

and Theoreme 3.1 in

[2],

to show that the

problem (QE)

admits -at least- one solution u E when E is "small"

enough.Using

the LP-estimates

(see [1]),

we infer that u E

W 2~p (SZ), Vp

> 1.

One can use

embedding

results

(see [8])

to deduce that u E

2. We show that if

(QE)

admits a

solution,

so does

(QE)

for every E E.

3.Using

the a

priori

estimate in

[6],

we show that

(QE)

does not admit a

solution,

if E is

great enough.

(10)

From these

steps,

we infer that the set I of E, for which

(QE)

admits a

solution,

is a bounded interval.

4. Let

f )

be the upper bound of I. The

blow-up argument

used in

[6],

can be

applied

to show that there exists no

increasing

sequence in

I,

such that

This last a

priori

~°°-estimate of the solutions uE near

E* (SZ, f ),

leads to a

solution of

(QE* (S~, f ) )

.

Remark 2. When SZ =

Br

-

~x

E

~’~; r ~

and

f(x,u)

-

ua,

then

l. every solution

of (QE)

is

spherically symmetric (see f5J),

2.

C2)

=

r 1 2a

E*

(B1, cx), (see ~10~~.

2.2. The

Supercritical

Growth Case

Let us consider the

following problem

We suppose that

(i)

Q is a bounded

regular domain,

which is

starshaped

about the ori-

gin.

(ii)

a E

R*+) and 03B2

>

n+2 n-2

.

Under

appropriate hypotheses,

the

following problem

admits solutions

(see [14]).

PROPOSITION 4. - Let us suppose that the

problem (P)

admits a so-

lution,

then under

hypotheses (i)

and

(ii),

there exists a

positive

constant

E*(SZ, a)

such that

(TE) admits,

at

least,

one solution uE E ,

0

b

1,

when 0 E

E*(SZ, a).

There is no LOO-solution

of (TE) for

E >

E*(S2, a).

(11)

Proof.

- The

proof

is similar to the demonstration of Theorem 2 in

[9].

.

Remark 3. - The

hypothesis concerning

the existence

of

a solution

of

(P) is justified by

the critical

growth

case

(see

section

1).

The

E* (SZ, a)-limit

case.

Before

dealing

with this case, let us state the

following

lemma.

LEMMA 1.2014 Under

the

hypotheses (i)

and

(ii)

, assume that is a

sequence

of C2 (03A9) - functions

and is a real sequence, such that

Then, if

the real sequence is bounded in

~,

so is in

Ho (SZ) . Proof. Using

Pohozaev

Identity,

we

get

Using

the Green’s first

identity,

we

get

So we infer that

Using

the maximum

principle,

and the fact

that uj

= , on

8Q,

we obtain

(12)

As f2 is

regular

and

starshaped,

we

get

where,

As,

we

get

where c2 0 c3 and ci, i =

2,

..4 are constants not

depending

on

j. Using

Holder’s

Inequality,

we obtain

Let us

put vj

=

then vj

E and

Using

Poincaré

Inequality,

we

get

As

t - J

and E~ is bounded in

~,

this

completes

the

proof

of Lemma 1. .

Remark 4. - The a

priori

estimate in Lemma 1 remains true

for

non-

linearities such

that,

there exist constants c

and 03B3,

with

(13)

PROPOSITION 5. Under the

hypotheses of Proposition ,~, if

a E

C°~~ (SZ),

0

~ 1,

then

(TE* (SZ, a))

admits a solution.

Proof.

Let be an

increasing

real sequence such that

For

every

let u~ be the solution of

(see Proposition 4).

As

u~ G

C2(O),

one can use Lemma 1 to obtain

Then,

up to a

subsequence,

u in - u in

L2 (SZ) -

strong

and uj ~ u, a.e. in SZ. One can

multiply (Pj) by

uj to

verify

that

By using

the Lp-estimates and a

bootstrap argument,

one can show that u is a solution of

(TE* (SZ, a) )

.

PROPOSITION 6. - Let u be a

spherically symmetric L~ (~n)-

solution

of

then u E and u E ,

Vp

>

ny 1 .

.

Proof.-

Let us choose r >

0,

such that

u(r)

oo. As u G

LOO(Br),

one

can use the LP-estimates

(see [1])

to infer that u E V p > 1. We infer that

(see [8])

From the

previous line,

we see that

u{3

E

C°~~(Br),

V 0 ~

1,

So we

can use the Schauder Estimates to deduce that u E We can use

Proposition 4,

to infer that

It is easy to

verify(

see

[10])

that

so we deduce

that, if p > n ~’ ~ 1 , then

u E .

Acknowledgments.

The author would like to thank Prof. A. Bahri and the Mathematics

Department

of

Rutgers University (USA)

for

hospitality

during

the fall 1998.

(14)

- 359 -

Bibliography

[1]

AGMON

(S.),

DOUGLIS

(A.)

and NIRENBERG

(L.).

- Estimates near the Boundary for Solutions of Elliptic Partial Differential Equations satisfying General Boundary

Value Conditions I. Comm. Pure Appl. Math., 12, pp. 623-727

(1959).

[2]

BOCCARDO

(L.),

MURAT

(F.)

and PUEL

(J.P.).

- Quelques Opérateurs Quasi-

linéaires. C. R. Acad. Sc. Paris, t. 307, Série I, pp. 749-752

(1988).

[3]

BREZIS

(H.)

and NIRENBERG

(L.).

2014 Positive Solutions of Nonlinear Elliptic Equa-

tions Involving Critical Sobolev Exponent. Comm. Pure Appl. Math. 36, pp. 437-477

(1983).

[4]

CRANDALL

(M. G.)

and RABINOWITZ

(P.H.). -

Some Continuation and Variational Methods for Positive Solutions of Nonlinear Elliptic Eigenvalue Problems. Arch.

Rational Mech. Anal. 58, pp.207-218

(1975).

[5]

GIDAS

(B.),

NI

(W.-M.)

and NIRENBERG

(L.).

- Symmetry and Related Properties

via the Maximum Principle. Comm. Math. Phys. 68, pp.209-243

(1979).

[6]

GIDAS

(B.)

and SPRUCK

(J.).

2014 A Priori Bounds for Positive Solutions of Nonlinear Elliptic Equations. Comm. Partial Differential Equations 6, pp.883-901

(1981).

[7]

GIDAS

(B.)

and SPRUCK

(J.).

- Global and Local Behavior of Positive Solutions of

Nonlinear Elliptic Equations. Comm. Pure Appl. Math., Vol.34, pp.525-598

(1981).

[8]

GILBARG

(D.)

and TRUDINGER

(N.S.). -

Elliptic Partial Differential Equations of

Second Order. Springer Verlag

(1977).

[9]

ISSELKOU

(O.A.-I.-B.).

- A Critical Value for the Boundary Datum of a Dirichlet’s Problem. Funkcialaj Ekvacioj 41, pp.207-214

(1998).

[10]

ISSELKOU

(O.A.-I.-B.).

2014 Donnéee au Bord Critique pour un Problème de Dirichlet.

Revue URED No 8 and 9

(Dakar, 1999).

[11]

JOSEPH

(D.D.)

and LUNDGREN

(T.S.). -

Quasilinear Dirichlet Problems Driven by

Positive Sources. Arch. Rational Mech. Anal. 49, pp. 241-269

(1973).

[12]

LOEWNER

(C.)

and NIRENBERG

(L.).

- Partial Differential Equations Invariant un- der Conformal or Projective Transformation. Contribution to Analysis

(L.

Ahlfors

ed.),

Academic Press, New York, pp. 245-272

(1974).

[13]

POHOZAEV

(S.I.).

- Eigenfunctions of the Equations 0394u +

03BBf(u)

= 0. Soviet Math.

Dokl. 6, pp.1408-1411

(1965).

[14]

POHOZAEV

(S.I.).

- On Entire Solutions of Semilinear Elliptic Equations. Research Note Math. 266, Pitman, pp.56-69, London

(1992).

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