• Aucun résultat trouvé

Séminaire Équations aux dérivées partielles – École Polytechnique

N/A
N/A
Protected

Academic year: 2023

Partager "Séminaire Équations aux dérivées partielles – École Polytechnique"

Copied!
8
0
0

Texte intégral

(1)

Séminaire Équations aux dérivées partielles – École Polytechnique

K. G. A NDERSSON R. M ELROSE

Propagation of singularities along gliding rays

Séminaire Équations aux dérivées partielles (Polytechnique) (1976-1977), exp. n

o

1, p. 1-5

<http://www.numdam.org/item?id=SEDP_1976-1977____A1_0>

© Séminaire Équations aux dérivées partielles (Polytechnique) (École Polytechnique), 1976-1977, tous droits réservés.

L’accès aux archives du séminaire Équations aux dérivées partielles (http://sedp.cedram.org) im- plique l’accord avec les conditions générales d’utilisation (http://www.numdam.org/conditions).

Toute utilisation commerciale ou impression systématique est constitutive 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

http://www.numdam.org/

(2)

S E M I N A I R E G 0 U LA 0 U I C - S C H W A R T Z 1 9 7 6 - 1 9 7 7

PROPAGATION OF SINGULARITIES ALONG GLIDING RAYS

par K. G. ANDERSSON et R. MELROSE SCOLB POLYTECHNIQUE

CENTRE DE

MATHEMATIQUES

PLATEAU DE PALAISEAU - 91128 PALAISEAU CEDEX

TéIéphone : 941.82.00 Poste N·

T6]ex : ECOLEX 691 596 F

Expose N0

I 19 Octobre 1976

(3)
(4)

I.1

R;f(x) &#x3E;0j

be a domain with

C 00 boundary

and

let P =

P(x,D)

be a second order differential

operator

of real

co -

principal type

with coefficients in C

(Q).

The

subject

of this lecture is to discuss the

singularities

of distributions u

satisfying

If P

denotes the set of zeros of the

principal symbol

then this

problem

has been treated

by

several authors

(see

We shall consider a case where

(1)

is violated. If the

boundary

ðO

is

non-characteristic,

then

We shall also assume

that Q

is

pseudo-convex

with

respect

to

P,

i.e.

The

opposite

case,

when Q

is

pseudo-concave,

has been treated in

LI-i

When

(2)

and

(3)

are

satisfied,

it is

possible

to define so

called

boundary bicharacteristics

for P as follows. Consider the

restriction

p

of p to the

symplectic

manifold

Lj ~p, f~ ( z) _ 01

The

projection,

onto of the null-bicharacteristics for

p are

called

boundary

bicharacteristics for P. It is easy to check that the null-bicharacteristics for the restriction of f to

give

the same curves as the null-bicharacteristics for

p.

In

fact,

the

tangent

of such a curve lies in the

plane spanned by Hp

and

Hf

and

is

orthogonal

to the

gradient

of

[p,f} .

(5)

I.2

In order to localize the

concept

of

"regularity

up to the

boundary",

we assume that Q is

given by x n

&#x3E; 0 and denote

points

on

the

boundary

6Q

by

x’ _

( x’ , 0) .

If we say that

u E H

at

(x’ ,~’ )

if there is a

homogeneous symbol W(x’ ,~’ )

such

that

*(xl F 1

1 in a

neighborhood

of

(xl

and

_ n

belongs

to H

s (11)

close to x’. Here it is

implicitly

assumed that

u(.,xn)

is well-defined. In the same manner we say that

_ n _ co -

if,

for some * as

above,

C

(Q)

close

to

x’.

This definition of microlocal

regularity

up to the

boundary

has also been

suggested by

Chazarain

[3J.

Theorem :

Suppose

that Q is

pseudo-convex

with

respect

to P and let

c - co-

if be a

boundary

bicharacteristic for P. If

u E ^’ ( ) , Pu E

C

(0)

and Y n 0.

then either

’l’ c WF(u~)

ory n

WF(u;Q) = ø.

Sketch

of proof :

: In order to avoid technical

complications,

we

only

consider the case when P is

hyperbolic.

We also assume that Q is

given by

x n

&#x3E; 0. Let

(x’ ,~ )

be a

point

where

tp,fl =

0 and denote

by

y =

Y~(x’ ,~’ )

the

boundary

bicharacteristic

through

the

projection

(xf I )

of

(x’ ,t )

onto

T~~ (8Q) .

The main

step

in the

proof

is to construct

a suitable

symbol a(x,~)

of order zero such that

and

a(x~p) =

1 on a conic

neighborhood

of

(x’~?).

Here the condition

(5)

is

required

to be satisfied for some choice of r and q.

If

(x* ~’)

is close to

(Xt9;-1)

then there is either no root

or else two roots

of the

equation p(x’p’ ) =

0.

These

roots

, n n

coincide when

tp,fl =

0. Since q is

independent

of r

n

it follows from

(5)

that one must have

Now

(4)

means that a is constant

along

the bicharacteristics for P so

(5’)

implies

that a has to be constant

along

the

successively

reflected

(6)

I.3

bicharacteristics. In

particular

it follows that a must be constant

along

the

lifting Y to 6.) n 1

of the

boundary

bicharacteristic r =

Y ( x’ , ~ ’ ) .

If we denote the flow-out

along

H

p

f rom Y ,

the results of

L7j imply

that a can be chosen to

satisfy (4)

and

(5)

and to have

support

in an

arbitrary

small conic

neighborhood

of

F(x’,F’).

Since

x n =

0 is

non-characteristic,

we can in

particular

assume that a has the transmission

property (see ,1

Let r be a

homogeneous symbol

of order -2 which has the trans- mission

property

and satisfies

(5)

and denote

by

R the

corresponding operator.

Let furthermore Q and A be

operators

with

symbols

q and

a + where

Here

p1

denotes the

symbol

of order one of P.

Assume now that

u E

H

s (0) along I

and

put

where

uo

denotes the extension of u which vanishes outside D. Since

y n

it follows from

(4) - (6)

that

Moreover

(5) gives

that

00

Because A and R have the transmission

property, Pu E

C

(0)

and

Y ~

we

get

from

(7)

and

(8)

that

If now some

point

on is outside

WF(u;R)

and

a ( x, ~ )

has

support sufficiently

close to

1 (x’ ,~’ ) ,

it follows that we can

oJ

assume that v has initialdata in C . Note that the

pseudo-convexity

(7)

I.4

means that the bicharacteristics in

r(’ ,’)

leave C2. Well-known

regularity

theorems for the mixed

problem

now

implies

that

Since

a(x,:) = q(xl 7 1 ) =

1 in a

neighborhood

of the zeros

of

p(x,~ ) ,

when

(x’ ,F’ )

is close and

x n is small,

we can

assume that

r (x,~ )

satisfies

there. Remember that

(5)

is

only required

to be satisfied when

x = 0. From

(9)

it follows that

n

close to Y . Thus

close to

~’ ,

and the

proof

is finished.

Remark : Just before this lecture we received a

manuscript

from

G.

Eskin where a

parametrix

is constructed for certain mixed

hyperbolic problems

with

gliding

rays. For second order Dirichlet

problems

such a

parametrix

has also been constructed

by

one of the

authors

(Melrose).

This construction as well as a fuller account of the

argument

described above will be

published

elsewhere.

REFERENCES

[1]

L. Boutet de Monvel : Acta

Math., 126, 1971, p.11-51.

[2]

J. Chazarain : Sem.

Bourbaki, exposé n° 432,

1973.

[3] J. Chazarain : Reflection of C~ singularities

for a class of

operators

with

multiple characteristics,

Publ. R.I.M.S.

Kyoto

Univ.

[to appear].

[4]

G. Eskin : A

parametrix

for the mixed

problems

for

strictly hyperbolic equations

of an

arbitrary order,

Comm. in Partial

Diff.

Eq. [to

appear].

(8)

I.5

[5]

G. Eskin : A

parametrix

for

interior

mixed

problems

for

strictly hyperbolic equations [to

appear].

[6]

R.

Melrose,

Duke Math.

J., 42, 1975, p.605-635.

[7]

R.

Melrose, Equivalence

of

glancing hypersurfaces,

Invent. Math.

[to

appear].

[8]

L.

Nirenberg :

A.M.S.

Reg.

Conf.

Series, 17,

1973.

[9]

M.

Taylor :

Comm. Pure

Appl.

Math.

29, 1976, p.1-38.

Références

Documents relatifs

Evans, Classical solutions of fully nonlinear convex second order elliptic equa-. tions,

of the Green function hold. Such estimates were obtained in [M-S] for uniformly elliptic operators on unimodular Lie groups and in [Kor 1,2] on general manifolds

of a (possibly new) proof of the classical Wiener lemma, which makes no use of Fourier transform or of abstract theory, and which might apply to other classes of

© Séminaire Équations aux dérivées partielles (Polytechnique) (École Polytechnique), 1970-1971, tous droits réservés.. L’accès aux archives du séminaire Équations aux

la construction du paragraphe 3) que toutes les ondelettes que l’on obtient à partir des analyses graduées en fonctions splines ont une

RUSSELL dans (Ru~, où il est prouvé qu’un résultat de contrôle exact pour l’équation des ondes entraîne le contrôle exact de l’équation de.. la chaleur ; or le

Solutions de viscosité des équations de Hamilton-Jacobi du premier ordre et applications.. Séminaire Équations aux dérivées partielles (Polytechnique)

quasi-complexe intégrable provient (localement) d’une structure quasi- complexe, au moins lorsque l’on fait une hypothèse de pseudo-convexité~. Il en est bien ainsi