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
o1, p. 1-5
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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 1976I.1
R;f(x) >0j
be a domain withC 00 boundary
andlet P =
P(x,D)
be a second order differentialoperator
of realco -
principal type
with coefficients in C(Q).
Thesubject
of this lecture is to discuss thesingularities
of distributions usatisfying
If P
denotes the set of zeros of theprincipal symbol
then this
problem
has been treatedby
several authors(see
We shall consider a case where
(1)
is violated. If theboundary
ðOis
non-characteristic,
thenWe shall also assume
that Q
ispseudo-convex
withrespect
toP,
i.e.
The
opposite
case,when Q
ispseudo-concave,
has been treated inLI-i
When
(2)
and(3)
aresatisfied,
it ispossible
to define socalled
boundary bicharacteristics
for P as follows. Consider therestriction
p
of p to thesymplectic
manifoldLj ~p, f~ ( z) _ 01
The
projection,
onto of the null-bicharacteristics forp are
called
boundary
bicharacteristics for P. It is easy to check that the null-bicharacteristics for the restriction of f togive
the same curves as the null-bicharacteristics forp.
Infact,
thetangent
of such a curve lies in theplane spanned by Hp
andHf
andis
orthogonal
to thegradient
of[p,f} .
I.2
In order to localize the
concept
of"regularity
up to theboundary",
we assume that Q isgiven by x n
> 0 and denotepoints
onthe
boundary
6Qby
x’ _( x’ , 0) .
If we say thatu E H
at(x’ ,~’ )
if there is ahomogeneous symbol W(x’ ,~’ )
suchthat
*(xl F 1
1 in aneighborhood
of(xl
and_ n
belongs
to Hs (11)
close to x’. Here it isimplicitly
assumed thatu(.,xn)
is well-defined. In the same manner we say that_ n _ co -
if,
for some * asabove,
C(Q)
closeto
x’.
This definition of microlocalregularity
up to theboundary
has also been
suggested by
Chazarain[3J.
Theorem :
Suppose
that Q ispseudo-convex
withrespect
to P and letc - co-
if be a
boundary
bicharacteristic for P. Ifu E ^’ ( ) , Pu E
C(0)
and Y n 0.
then either’l’ c WF(u~)
ory nWF(u;Q) = ø.
Sketch
of proof :
: In order to avoid technicalcomplications,
weonly
consider the case when P ishyperbolic.
We also assume that Q isgiven by
x n
> 0. Let(x’ ,~ )
be apoint
wheretp,fl =
0 and denoteby
y =
Y~(x’ ,~’ )
theboundary
bicharacteristicthrough
theprojection
(xf I )
of(x’ ,t )
ontoT~~ (8Q) .
The mainstep
in theproof
is to constructa suitable
symbol a(x,~)
of order zero such thatand
a(x~p) =
1 on a conicneighborhood
of(x’~?).
Here the condition(5)
isrequired
to be satisfied for some choice of r and q.If
(x* ~’)
is close to(Xt9;-1)
then there is either no rootor else two roots
F±
of theequation p(x’p’ ) =
0.These
roots, n n
coincide when
tp,fl =
0. Since q isindependent
of rn
it follows from
(5)
that one must haveNow
(4)
means that a is constantalong
the bicharacteristics for P so(5’)
implies
that a has to be constantalong
thesuccessively
reflectedI.3
bicharacteristics. In
particular
it follows that a must be constantalong
thelifting Y to 6.) n 1
of theboundary
bicharacteristic r =Y ( x’ , ~ ’ ) .
If we denote the flow-outalong
Hp
f rom Y ,
the results of
L7j imply
that a can be chosen tosatisfy (4)
and(5)
and to have
support
in anarbitrary
small conicneighborhood
ofF(x’,F’).
Sincex n =
0 isnon-characteristic,
we can inparticular
assume that a has the transmission
property (see ,1
Let r be a
homogeneous symbol
of order -2 which has the trans- missionproperty
and satisfies(5)
and denoteby
R thecorresponding operator.
Let furthermore Q and A beoperators
withsymbols
q anda + where
Here
p1
denotes thesymbol
of order one of P.Assume now that
u E
Hs (0) along I
andput
where
uo
denotes the extension of u which vanishes outside D. Sincey n
it follows from(4) - (6)
thatMoreover
(5) gives
that00
Because A and R have the transmission
property, Pu E
C(0)
andY ~
weget
from(7)
and(8)
thatIf now some
point
on is outsideWF(u;R)
anda ( x, ~ )
hassupport sufficiently
close to1 (x’ ,~’ ) ,
it follows that we canoJ
assume that v has initialdata in C . Note that the
pseudo-convexity
I.4
means that the bicharacteristics in
r(’ ,’)
leave C2. Well-knownregularity
theorems for the mixedproblem
nowimplies
thatSince
a(x,:) = q(xl 7 1 ) =
1 in aneighborhood
of the zerosof
p(x,~ ) ,
when(x’ ,F’ )
is close andx n is small,
we canassume that
r (x,~ )
satisfiesthere. Remember that
(5)
isonly required
to be satisfied whenx = 0. From
(9)
it follows thatn
close to Y . Thus
close to
~’ ,
and theproof
is finished.Remark : Just before this lecture we received a
manuscript
fromG.
Eskin where aparametrix
is constructed for certain mixedhyperbolic problems
withgliding
rays. For second order Dirichletproblems
such aparametrix
has also been constructedby
one of theauthors
(Melrose).
This construction as well as a fuller account of theargument
described above will bepublished
elsewhere.REFERENCES
[1]
L. Boutet de Monvel : ActaMath., 126, 1971, p.11-51.
[2]
J. Chazarain : Sem.Bourbaki, exposé n° 432,
1973.[3] J. Chazarain : Reflection of C~ singularities
for a class ofoperators
withmultiple characteristics,
Publ. R.I.M.S.Kyoto
Univ.
[to appear].
[4]
G. Eskin : Aparametrix
for the mixedproblems
forstrictly hyperbolic equations
of anarbitrary order,
Comm. in PartialDiff.
Eq. [to
appear].I.5