A NNALI DELLA
S CUOLA N ORMALE S UPERIORE DI P ISA Classe di Scienze
A LDO A NDREOTTI C. D ENSON H ILL
E. E. Levi convexity and the Hans Lewy problem. Part II : vanishing theorems
Annali della Scuola Normale Superiore di Pisa, Classe di Scienze 3
esérie, tome 26, n
o4 (1972), p. 747-806
<http://www.numdam.org/item?id=ASNSP_1972_3_26_4_747_0>
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AND THE HANS LEWY PROBLEM.
PART II : VANISHING THEOREMS
by
ALDO ANDREOTTI and C. DENSONHILL(*)
In Part I of this work
[6]
we introduced certaincohomology
groups, and showed howthey
are connected with theCauchy problem (or
H.I,ewy problem)
and the Riemann-Hilbertproblem,
forcohomology
classes and theoperator
~. In this paper wegive
localvanishing
theorems for these groups atboundary points
oflocally
closedregions, partially
boundedby
a smoothhypersurface
inGn.
These theorems(Theorems
1 and2)
show that it ispossible
todecide, according
to the E. E. Leviconvexity
of thehypersur- face,
whether or not theproblems
mentioned above arelocally well posed.
Global
vanishing
theorems or theorems of finiteness can be deriveddirectly
from the localvanishing
theorems(n. 18). Also, global Cauchy
orRiemann-Hilbert
problems
can be treated once theglobal
finiteness theo-mes have been
acquired (cf.
n.19).
Therefore we have refrained from set-ting
up all themachinery
necessary for a directproof
ofglobal vanishing
theorems or theorems of
finiteness ;
we have concentrated our attentionon the local situation. This can be handled with some
simplifications
with
respect
to thegeneral
case.We have followed
partly [4]
andpartly
the paper of L. R6rmander[7].
It should be
pointed
out that essential use is made(as
isrequired by
thenature of the
cohomology
groups wetreat)
of theregularity
theorem of J.J. Kohn and L.
Nirenberg [8].
These results have been announced at the International
Congress
ofMathematicians,
in Nice(1970), by
one of the authors.Pervenuto alla Redazione il 12 Maggio 1971.
(1.) Research supported by the Office of Scientific Research of the United States Air Force under Contract AF F 44fi20-72-C-0031, and by the North Atlantic Treaty Organization during the term of a Postdoctoral Fellowship in Science.
1. dnnalv della Scuola Norm. Sup. di Pisa.
The reader should refer to Part I
[6]
for any notation notexplained here,
for the definition of thecohomology
groups weemploy,
y and for themotivation behind this work.
§
1.Pt8elilllinaires.
1.
Sequences of
Hilbert spaces anddensely defined operators.
a)
For the sake ofcompleteness,
we first recall some well-knownfacts. Let
Hi
and.g2
denote two Hilbert spaces and let D be a densesubspace
of.H~ .
be a linear map and let
be the
graph
of t. LetGt (D)
be the closure ofGt (D)
in theproduct topo- logy
of and ThenGt (D)
is a linearsubspace
of81
X~2 .
If
Gt (D)
is thegraph
of a(necessarily linear)
map T from the spaceGt (D)
we say that t defines adensely defined
closed linearoperator
with domain
DT
andgraph GT = Gt (D).
We will call T the closure of t withrespect
to D.EXAMPLE : Let t be a differential
operator
t =P (x, D)
with C °° coef- ficients defined on an open set LetCJ) (A)
be the space of C °°functions with
compact support
in A and letH2
= E2(A,
wheredl4
isLebesgue
measure. Let be a space of squareintegrable
C °°functions on A such that t defines a linear
operator
t :D -~ H2 .
The closureof
Gt
is still thegraph
of a linear map T. For this it isenough
to showthat if I are two sequences in D both
converging
to an ele-ment xo E and if t
(x,) (xy)
-+yo’ ,
then we musthave yo
=yo
·Denoting by (, )
the scalarproduct
in.L2 (A, dft)
weget
for everywhere
tP (x, D)
denotes the formaladjoint
ofP (x, D).
The condition(yo
-yb f )
=0, V (A), implies yo
=y’
since(Z) (A)
is dense inL2 (A,
Of course the closure T of the
operator t depends
upon the choice of the densesubspace
D.b)
LetT : H1.., ---~ H~
be a closeddensely
definedoperator.
We setsuch that ’ °
Since
DT
is dense inHi
the(adjoint)
linear map which associatesT*g
=g-
to g, is well defined.If RTe consider in
Hi X H2
the hermitian formfor U = U1
X u2
and V = v,X v2 ,
then we can describe thegraph
of T*as folluws :
This shows that T* is a closed
operator,
itsgraph being
theQ orthogonal complement
ing1 X H2
of thegraph GT
of T. From this it follows thatGT ix,
inturn,
theQ.orthogonal complement
ofGT~
and therefore we de- duce thatT* is
densely
defined with domainDT*
and that T** = T.The
following
are obviousproperties
for the closeddensely
definedoperator
T:In
particular,
THEOREMI A. Let T :
H,
... -.g2
be a closeddensely defined operator.
The
following
conditions areequivalent : a)
Im T is closed.b)
There exists a constantc ~
0 such thatc)
ImT* is
closed.d)
There exists a constant c > 0 such thatThe best constants in
b)
andd)
are the same. We have borrowed this theo-rem from Hbrmander
[7] (p. 91,
Theorem1.1.1).
c)
DIEFINITION. Acomplex of Hilbert
spaces and closeddensely defined.
operators
is a sequenceof
Hilbert spaces and closeddensely defined operators Ti :
such
that, for
each i EZ,
we have ImTi,
C KerTi+l .
Inparticular,
a shortcomplex
is a sequencewith
J7g
Hilbert spaces and T and S closeddensely
defined and such that Im T c Ker S.Replacing
theoperators
in(a) by
theiradjoints
weget
a newcomplex (the adjoint complex)
Indeed,
Ker T* =(Im (Ker S )1=
ImS*.
Thefollowing
theoremgives
a criterion foracyclicity,
i. e., forhaving
THEOREM B. Assume that
for
thecomplex (a)
we canfind
a constantc > 0 such that
Then
(a)
ImT,
ImS,
1mT*,
ImS*
are all closed.(b)
Thecomplex (a)
isacyclic,
Im T = KerS; for
g E Ker S we canf ind
u EDT n
Im T* such that(c)
Theac7joint complex
isacyclic,
Im ~5~ = KerT ~ ~ for
g E Ker Tffwe can
find
u EDs*
tl 1m S such that(d) If
h E Im ~’ ~ we canfind
v E Ker S such that(e)
E Im S we can E Ker T* such thatConversely if
thecomplex (a)
isacyclic
and Im S isclosed,
thenfor
someconstant c > 0
inequality (1)
must hold.PROOF.
(a)
!f it followsfrom
(1) that g || g || c2||
. Thusby
TheoremA,
Im S is closed and2 3
Im S* is closed.
If g E DT* n (Ker
cDT*
n(Im T )
cDT
y from(1)
weget
|| I g I g || c I
. Thusby
TheoremA,
Im T* is closed and Im T is2 1
closed.
(b) Let g
E Ker S. To showthat g
E ImT,
it suffices to show that there exists a u E.~1
such thatIndeed,
thenu E DT** = DT
and thereforeSince
DT*
is dense inH2,
it follows from(Tu, f ) _ (g, f )
that g = Tu.Since we can write
jDy. = (Ker ®
Now
if f E Ker S1,
we have(g, f ) = 0
andT ~f = 0
since(Ker 8)1
C Ker T*.then
by (1)
we haveThis shows that if
f E
KerT*,
then(g, f ) = 0 (1)
and therefore we can con-(i) We can write f = f1 + f, with f, E (Ker
S)1
and 12 E Ker ,S n Since f and Iiare in Ker T *, so is 12. We then have
(~/)=(~/i)+(~,/2)=~
because (g, fi) = 0,and for f2 we have .
sider
(g, f )
as a linear functional on Im T*. Moreover we havefrom what we have
just
said. Thus(g, f )
as a linear functional on Im T*is
continuous ;
hence there exists a u E Im T ~ with such that(9~ .f ) _ (u, ~’~f )~
(e)
isproved
as in(b).
(d )
From(b)
we have now that Im T = Ker S and Ker T ~ =(Ker 8)1.
·Thus If
h = T*u, u E DT*’
we can write2c .--- oc
-~-- v
witha E Ker T "
and v E Ker S nDT*.
Then we have h = T ~vand from
(I) ) ) v ] ]2 c2 ) ) T~v~~2=c2 ~h~~2.
(e)
is the same as(d).
It remains to prove the converse
part.
First we remark that from Im T = Ker S it follows that(Im T)1= (Ker 8)1. Hence, using
Theorem Aand the fact that Im S is
closed,
weget
that theadjoint complex
isacyclic:
= Ker T*.
Secondly,
we haveThus
DT*
= Ker ~’~ flDs EB
Ker S nDT* (indeed,
if u+ v
EDT*
withu E Ker T*,
andif u + v E Ds, then,
sincev E Ds,
we musthave u E Ker T * t1
Ds ). Let g
EDs
(1Dp* , 9
= u+ v according
to the ortho-gonal decomposition given
above. We Alsoby
Theorem A we must have
Adding
these twoinequalities
we obtaininequality (1).
REMARK. An estimate of
type (1)
is called aW ellipticity
estimate(cf.
[4], [5]).
Thevalidity
of aW-ellipticity
estimateimplies
forHi,
1~2 , .B3
the
following
direct sumdecomposition
into closedsubspaces
COROLLARY. Assume that a
W-ellipticity
estimate(1)
holds. Thengiven f E .H2
withf E
KerS,
there exists aunique
u in.gi
with u EDT n
1m T ~ anda
unique
x in.g2
with x EDT*
fl Ker S such thatMoreover,
we have the estimatesand
therefore
An
analogous (adjoint)
statement isvalid,
in which theS, T, S*,
T* are re-placed, respectively, by T*, S*, T,
S.PROOF.
By looking
at the above direct sumdecomposition
we see:since
f
E KerS,
thenf
E 1mT;
i hence for some u EDT,
Tu= f:
The choiceof u is
uniquely
determinedby requiring
that and fromthe
previous
theorem(b)
weget
the estimate11 u c II f IIHi.
· But(Ker T )1=
Im T*. Thus there exists an x EDT-
such that u = The choice of x isuniquely
determinedby requiring
that= Ker s n
DT- -
Hence Sx = 0 andby
theprevious
theorem(d )
weget
theestimate
Now
S*Sx
= 0 since ~x =0 ;
therefore2. Notation and
preliminaries. a)
Let U be an open set in wherez =
(zl
... ,zn)
will denote the usualholomorphic
coordinates.For u, v
inC~~°s~ ( U ~,
we define the
pointwise
euclidean innerproduct
and the
pointwise
euclidean normIf we want to
emphasize
thesystem
of coordinates we havechosen,
we will
write
insteadI2.
Another choice of
holomorphic coordinates ~
=(~l ,
... ,,,)
on U willproduce
anequivalent
norm on anycompact
subset ..~ ofU;
i. e., we can findpositive
constants°1 (K), C2 (K)
sueh that for anypoint
ofK,
We fix the volume element
and define the *
operator.
* :( ~T )
-0/::-8,
n-r)(U), by requiring
thatOne has
b)
Letfunction ;
we set’
and we assume that
dh #
0on S,
so that S is a smoothhypersurface.
Note that Q may bepartly
open andpartly
closed.(2) The
prime
denotes summation over strictly increasing multi-indices,Let u, v
be forms in(S~)
such thatis a
compact
subset of ,~. We then defineIf u E
(’0)~ ~
E(Q),
and if the intersection of theirsupports
iscompact
inQ,
we obtain from Stokes formula the relationwhere
We want to
investigate
under which conditions theboundary integral
in
(1)
vanishes.For that purpose, we introduce the differential
ideal 9°°
=E9 9’:: 8)’
where
and we denote
by ~~~r, ~~ (S~)
thesubspace
of9«o> (Q) consisting
of thoseelements with
compact support
in Q. We maydrop
thesuperscript
oo whenit is obvious from the context.
LEMMA 1. Consider the
equation
for f
ECp~r, ~_1) (~~)
and g E0(n--r,
n-s)(Q).
a)
The necessary andsufficient
conditionfor (2)
to holdfor
any choiceof f
is that g E1°>.
b)
For g tobelong
to9t:-r,
n-s)(S2),
it isenouyh
toverify
thatequation
(2)
holdsfor
a,ll f E~,~p~n-r, n-s-~-1) (Q).
PROOF.
Sufficiency. Let g
= ha+
Bh with a E(~)
and(3
E n-I-1)(Q).
Since h = 0on S,
weget
Now if i : S --~ ~I is the natural
injection,
l*dh =(h)
= dO = 0. Thusthe last
integral
is zero because dh on S is zero.Necessity.
It isenough
to prove statement(b)
i forthat,
it isenough
to show
that g
E5~~,~-~
in a smallneighborhood
OJ of eachpoint zo
E Sin U
(by using
apartition
ofunity).
Ifsufficiently small,
we may assume that h can be taken as a coordinate in asystem
of local C °° coordinateson OJ.
Let
f
becompactly supported
in w, andset,
for 8 small andpositive,
Then F
(E)
is a 01 function in a small interval 0 C 8 2 and we haveFrom the mean value theorem we derive:
for some
moreover,
Therefore,
iff
is of the abovespecified type,
we must haveLet I
be a real C °°function, compactly supported
in m, with0==~~1
and ~ ~ 1
in aneighborhood
w’ ce w of zo. Thenand therefore we must have
because fAg A
ah = alv12 dp.. Again by
themean value theorem we
have,
for some E’ with 0s’ E,
When E -~
0,
then 8’ --~0,
and we deduce thatTherefore, , I 9
A ahI2
= 0 on S andconsequently
in aneigbborhood of zo ,
According
toProposition
1.2 of[6],
thisimplies
that g E9(n-r,
n-s)(lJ
flw’).
As a
corollary,
we deduce thefollowing
PROPOSIZITON 1.
(a) If
v EC°°, 8 (,Q),
andif for
every u E iaehave
(b) If
u E(Q),
andif, for
every v ECo~r, 8~ (Q),
we havethen u E 8-1)
(Q).
-
REMARKS 1. The condition is
already implied by
thevalidity
of(au, v)
=(u, lsv)
for all u E _2. The condition u E
~
isalready implied by
thevalidity
ofv)
==
(u, Ov)
for allv E 9.
c)
Let 0 : Q - R be a C °°function;
for u, v inC~r, _~
with(support of u)
f1(support of w) compact,
we define theweighted
scalarproduct
and for
compactly supported u
we set11 u 11’45
=(u, u) !P
We call 0 aweight
on the space
C(,,,) (0).
The formaladjoint
withrespect
to this scalarprod-
uct of the
operator ~.===~-==2013
~ J is theoperator 61
’and the commutator is
given by
If we introduce the
weight ø 1
on the space(Q)
and theweight
tP2
on the spaceC~)(J3~
weget
as formaladjoint
of theoperator
a :
--~(~)
the differentialoperator :
d)
Given the functions 0 and hon Q,
for every z EQ,
we will makeuse of the
following
notations :For u E
(S~),
weset,
when s ~1,
and
n
1
n 2
where I grad k [ = 2 1 12
2
is the euclidean norm of the
gradient
of
h,
calculated at z.e)
We end thisparagraph
with someexplicit
formulas we need inthe
proof
of the basicestimatei :
Let
where A =
(Ctf ,
... ,Ctr),
B ====(~ .,. , Ps).
We denote - the
partial
derivative andby a-
thepartial
derivative
We have
where C
= y1,
,., ,ys+1).
If D denotes a multi-index oflength s -1 ~
we haveIn
particular,
and if we set
01 =- 0 - 2y), 02 == ø - 1jJ,
weget
Finally,
the condition u E*i7
isequivalent
to the condition§
2. TheEstimates.
This section is devoted to
establishing W-ellipticity
estimates for thea-operator
andboundary
estimates needed forregularization
ofLz-solutions.
3.
Stretching
the coordinates. Let 0 be a C °° function defined in someneighborhood U
of apoint zo
E(tn.
We assume thatat zo
the Leviform (zo)
has atleast p positive eigenvalues.
By
aunitary
transformation we can assume that isdiagonalized
at the
point zo
witheigenvalues
so that
We now
change
thecoordinates,
firstbringing zo
to theorigin by
atranslation and then
applying
the transformation z- 1 :
withIn the new coordinates we
get
and therefore
provided u
is oftype (r, s)
with s > ~2013~; infact,
everycomponent
when J contains more than n - p
indices,
must have one of the indices1~...~
among the indicesappearing
in J.We can therefore find ?7o
>
0and so >
0 such thatif q > then,
in the ball
B (zo) _ (~ ~ ~~ ~Q S Eo~,
we have for any withNow
let a
be a C °° function defined on1R
with theproperties:
If we
set ii§
=,u(Ø)
weget:
We thus obtain the
following
PROPOSITION 1. Let 0 be a C °°
function defined
in an openneighbor-
hood U
of
zo z7z~’~,
and such that,~ ( ~) (zo)
has atleast p positive eigenva-
lues. Then we can
find
-i)
aneighborhood
roof
zo with w cU,
ii)
asystem of holomorphic coordinates ~
inU,
such thatfor
any C°°function
p:1R
-1R
with~C’
~0, ~u"
~ 0 and arcy u E( IT)
withs >
n -_p,we have
In
particutar, for
p(t)
_--_ t we have4. Choice
of
theweight functions
and basicinequality. a)
We assume inthis section that D is
compact,
so that S =aD
is acompact
smoothhy- persurface.
Let us consider a C °° vector field
(complex-valued)
on U :Setting
we have the formula
On S we define the
quantity
Then we have the formula
where dS denotes the element of area on S oriented in such a way that
dft
= dS Adg, where g
= 2013( 12) 2
h. We denoteby div
thep
b)
Given the form with we construct the vector field on Dwhere
A direct calculation establishes the
following
basicidentity (cf. [5],
p.113).
valid for any choice of 0 and for any u E with s ~ 1.
The calculation is based on the
computation
of thedivergence
of thevector
field 8, making
use of the Ricciidentity (n. 2),
and theidentity
LEMMA 2.
If
u E(Q),
then thevector field
0 h-aa thefollowing properties :
1 W
PROOF. Let c
= -
2(2* aah 12) 2.
Then we have.11
= - e!t
eL (h) lu, ti) (again by
virtue of formula(5)
of n.2).
Making
use of thislemma,
and theprevious
basicidentity (4),
we obtainPROPOSITION 2. For any u
E *9 (Q)
fl we have thefollowing
identity :
Here we have
changed
theweight 0
into- 1>,
so as to have the firstterm on the left with the
positive sign.
c)
For the spaceswe now select the
weights
as follows :on
F3
we choose theweight ø,
on
FQ
we choose theweight ~2 = ø - 1jJ, on F1
we choose theweight ~1= ~ - 21jJ,
where 1jJ
is a C °° function on U. FromProposition
2 we derivePROPOSITION 3. For any u E we have the
following inequality :
PROOF. We have to compare
,0-w
withø1{}-ø,.
From formula(4)
ofn. 2 we obtain .
From the
inequality a -fi b ~2 C 2 ~ a ~2 -~- 2 b ~2
we derive the estimate2. Annali della Scuola Norm. Sup di Pisa.
Multiplying by
e-lp andintegrating
over D we obtainThis proves
Proposition
3.5. Local estimates in the interior. Let U and 4ii be as
before,
with iiicompact.
Select a function 4l that is
strongly plurisnbharmonic
in Q.Replacing
4l where p :
1R
is C °°increasing (p’
h0)
and convex(ft"
~0),
we may assume that for every u E(Q)
with s >1,
we haveFrom
Proposition
3 we thus derive thefollowing
PROPOSLTION 4. We can choose a
strongly plurisubharmonic function 0
on Q such that :
for
any choiceof
a C °°increasing
convexfunction
,u on1R,
and~ 0
for
any choiceof
u E(Q),
with s ~1,
we have
°
Here
6. Local estimates at the
boundary.
Let U be open in(tn
and let Q == (x E
where h is 0- and(x E
We want to prove the
following :
PROPOSITION 5. Let zo E S and assume that
(zo)
has at l east p po-sitive
eigenvalues.
Then there existsi)
an openneighborhood
OJof
zo inU, ii)
asy8tem of holomorphic
coordinates inU,
iii)
astrongly plurzsubharmonic function (P
on co, such that : For anychoice
of
anincreasing
convex 000function
p on1R,
andfor
any u E nS~)
nn
(w
flQ)
with s>
n - p, we have on w f1Q,
Here
03 = IU (0), ~2 = ,u ( ~) - y~, 01 =,a (0) - 2y,
and the above e,xpres- sion iscomputed
in the coordinatesystem given by ii).
PROOF. We
apply Proposition
1 to the functionh ;
there is an openset w 3 zo , and there are
holomorphic coordinates C
on U suchthat,
on OJ,for any 1t E
*9 n (w
nS~)
with s ~> ~ 2013 p.Now choose P as was done in
Proposition
4(replacing
Qby
wthere)
so that
The estimate then follows from
Proposition
3.REMARK. We may select (JJ to be a domain of
holomorphy
and Pstrongly plurisubharmonic
in w such that the sets~x E w I ~ (x) c~
arecompact
in w for every c E1R (i.
e., ~ : w -1R
is a propermap).
COROLLARY. Under the
assumptions of Proposition 5,
C °°function
in w we can choose theincreasing
convexfunction fl
such thatfor
~3 = ,~ ~ ~)~
andfor
I1
(w
nQ)
with s) 7i
- p, we haveif
a) aitd 0 are as in theprevious remark, given
anyJ* E
E
(w
fl we can select ju such thatPROOF. For the
validity
of theinequality (a),
a must be chosen such thator
This is
possible
since the second member is a bounded function on any set~~k-~-1~
for ~==1, 2,....
For condition
(~)
it isenough
to choose Itincreasing
convex such that7.
Symmetrization of
theiceights.
Since the paper of Kohn and Niren-berg employs only .L2-norms
withoutweights,
we show how to write thebasic estimates
using only L2-norms
andputting
anequal
share of theweight
on each of theoperators a
and 0.For notational convenience we
replace
theweight
functions01
7 Yby 2 ~1,
72 ~2 ,
7~~3’
For anypoint
wheref (h) (zo)
has atleast p positive eigenvalues,
we can select an openneighborhood
coof zo
which isa domain of
holomorphy,
a C °°funtion 1p
on co, and astrongly plurisub-
harmonic proper function 0 :
OJ -+ 1R
so that we have the estimate(for 2~g
=ø, 2Ø2 2Ø{
= 4l -21p)
for all u
(w
fl~3)
fl(OJ
fl£2)
with s>
it - p.Let us denote
by
D the set ro n Q. If aand P
are C °° functions onD,
we will use thefollowing
notation :We then have the commutative
diagrams :
and
Applying
theisomorphisms
we deduce from
(1)
thefollowing inequality
on D = (M fl Q :This is valid for all 1t E
*9 (D)
nCo~~, 8~ (D)
with 8] n - ~.
Moreover, given
anyf E (D)
the choice of (P can be made such that forf’
=e-’2 f
we have-
We note that the
problem
offinding
a solution tois
equivalent
to theproblem
offinding a
solution to§
3.Vanishing theorem
for Hr,8(D).
8. Preliminaries.
a)
The situaticn we areconsidering
in thefollowing :
On an open set U of
Gn
we have a C °° function h : ~ --~1R;
we setand we assume that
dh #
0on S,
so that S is a smoothhypersurface.
Let
z E S ;
we assume that(zo)
has atleast p positive eigenvalues.
Then
according
toProposition
5 we can choose the coordinates inwe can find an open
neighborhood
w of zo in U which is a domain of ho-lomorphy,
and we can choose a 000strongly plurisubharmonic
function0 : w -
1R
which is proper and such that:for any choice of a C °°
function 1jJ
on wfor any choice of an
increasing
convex 000function a
on1R
we havean estimate
for any u
Q)
flCo~r, ~~ (w
flQ)
with s ) ~z - p.. We remark that any
sufficiently
small domain ofholomorphy
w whichcontains zo
will have thisproperty.
In any case, w will be assumed bounded.b)
We fix w and set Let be a sequence of real- valued C °° functions on w such that:i)
~y hascompact support
inw, V
v E Nii)
for anycompact
subset .g c w there is an suchthat fJ"
== 1 on K if ’)1(K).
We choose now the
function 1f’
to be C °° on w and such that:for
v =1, 2~ 3~
....This
function 1jJ exists,
since on anycompact
set I~ there isonly
a finite set of v’s such
that ~
0 on K.We then choose the function ø as stated above and we take the
weights
be
given.
Then we can select thefunction f1-
in sucha way that we
have, according
to thecorollary
ofProposition
5 and(n. 7).
the
Basic estimate on D :
for
all u E*9 (D)
with s>
n - p ; moreover,where
c)
We now defines the Hilbert spaceswhere denotes the closure of with
respect
to theusual L2-norm
(without weight).
Next we define the
densely
defined linearoperators
as follows :
T is the closure of the
operator
S is the closure of the
operator
Since
we
obtain,
whenclosing
thegraphs,
thatIn conclusion we
get
a shortcomplex
of Hilbert spaces anddensely
defined closed
operators :
PROPOSITION 6. For the above
defined
short we havePROOF.
By
definition(D)
cDT
and(D) c Ds;
hencei)
andii)
follow.Let this means that for every zc E
C2013i)(-D)
we0
have
(Tu, v)
=(u, T*v),
inparticular
for every 2c EVO(:.,8-1) (D).
Now on
(D)
T isgiven by
the differential I sothat we
have,
for u ECo~~, ~_1y (D), v E (D),
0
In
particular,
for every u E(D)
we obtainThis shows that if and v E
C~~r, $~ ~D~,
we haveBut then from
(a)
it follows that we must haveAccording
toLemma 1~
thisimplies
thatConversely,
because of(fJ),
if
v E ~.~,
thenagain by
virtue of that lemma. This provesiii).
The
proof
ofiv)
isby
the sameargument. Finally, v)
follows fromii)
and
iii).
REMARK. We have shown that
9.
Density
theorem.a)
Consider thedensely
definedoperator
For u E
Dr*
f1Ds
we defineas the «
graph
norm >> for T~ x S.We have the
following density
theorem :THEOREM 0. The space
*9tD)
n00(:., s) (D)
is dense inDT* il DS
in thegraph
norm.PROOF. Consider the sequence q, defined in the
previous
section.Let u E
Dr*
nDs.
Then rjy u EDr* n Ds
for each v. For this it isenough
toshow that
i)
if u EDs ~ then
?i Eii)
if 1t EDT* ,
EDT* .
we
have u EDs
andFor we
u EDs
andFor v E
00(:.,8-1) (D),
we have v EDT
andLet
u E Ds.
We can find a sequence with~M2013~~2013~0
and‘I
Su - 0. Then remains valid also in thelimit ;
2c EDs .
Let
Then, °° D
for any v ECo., s_l )
we we havehaveFrom this we
obtain,
for v EDT
Hence the functional
I (v) = (,q,, u, Tv)
iscontinuous,
extends to all ofand we can write
for some
g E Hi.
This shows thatqv u E DT * (and
T ~(r¡,,1l)
=g).
(b)
From the lastargument,
because of the choiceof q,
we haveHence there exists a constant c >
0, independent of v,
such thatfor every 2c E
.DT~
and E(D).
Consequently
we must haveBy
a similar andsimpler argument,
we deduce from(a)
thatwith another constant c
>
0independent
of v.(c)
We now showthat ||nv 1t 111-+
0 as v -> oo.1.
pointwise
onD, I ~v u - ~c I2 C I ~c 2 and II 1~ II2 C
00.Therefore
by
theLebesgue-dominated
convergence theorem we obtain thatas
2. - SIt
II ~ I I ~ ~~y 1t) + 11
The second term on the
right
tends to zeroby
the sameargument given
for 1. The first goes to zero as v -~ oo, because vol
(supp 1 2013~
0.Both terms tend to zero as v - oo
by
the samearguments
as thosegi-
ven in 2.
(d)
We can therefore suppose that it EDT* fl Ds
hascompact support
in D. We want to show that we can find a sequence with
such as k - 00.
Let D’ be a subset of
D,
open inD, relatively compact
inD,
andsuch that supp u C D’. Let co’ be an open set in (o such that D’ = D n
00’,
and therefore I)’ =
ix
E00’ h (x)
~0).
We now consider on D’ thesystem
of
equations
where
f =
S-uand g
= T *uby
definition. If we extendu, f, g
to onw’
by setting
themequal
to zero on w’ -D’,
then since 2c EDT~ ,
for anyv E
(w’)
we haveNow the
system (s)
is of thetype
studiedby
H6rmander[7] (3)
and« the
Cauchy
data of u withrespect
to theoperator
T* vanish on h = 0 ».(3) Note that the system has the form
with B and C of order zero with C °° coefficients that are bounded on D’; 1jJ, B, C can
be extended in a C °° fashion, keeping them bounded on w’,
Therefore,
we canapply
to(E)
theproposition
1.2.4 of his paper and deduce that there is a sequence uk E(D’~~
( lc =1, 2, 3, ...)
such thatand moreover zck E
DT. (D’) ; i, e. , (D’).
This com-pletes
theproof of
the theorem.b)
As an immediate consequence of thedensity
theorem we derivefrom the basic estimates the
following important
COROLLARY 1. For the short
coinplex of
Hilbert spaces and closed den-sely defined operators,
we have aW-ellipticity
estimatewhenever s > n - p.
From this
corollary
we obtain that if s > 11, - p thegraph
normIII II
is
equivalent
to the «Dirichlet norm >>Now let us remark that under the
graph
norm the domain of a closeddensely
definedoperator
is acomplete
space. Inparticular, by applying
these remarks to the
operator
T*X S,
whose domain isDr* n Ds,
weget
the
following
Then if
s>
it - p, thecompletion
Kof
the space B withrespect
to theform
1
Qo (u, u) 2 is
the space K =DT*
flDs.
c)
Now letp E S
~1 D and consider anyneighborhood
of p in Usuch that w’ n D is
compact.
Set D’ =D’ (p)
= D.Then from the basic estimate we deduce the
following
COROLLARY 3. Let a
point p E ,S ft
D and arelatively compact neigh-
borhood D’
( p) of
p in D begiven.
Then there exists a constant c(D’) >
0such that
for
all u E B(D’)
=.9 (D’)
fl(D’)
with s > n - p.10. The
vanishing
theorem.a)
We formulate thevanishing
theorem asfollows :
THEOREM 1. Let U be open in
Gn,
let h : U -+1R
be a 000function
with
~x E
Letzo E S
bea point of
S at which-0 (h),
the Leviform of h,
has at least ppositive eigenvalues.
Then there existsa
neighborhood
Wof
zo in U such thatfor
any domainof holomorphy
(ocontained in
W, setting
D =(x
E wI
h(x) 0 ),
we haveREMARK. What
really
has ageometric meaning
is the number a ofpositive eigenvalues
of the Levi form restricted to theholomorphic tangent
space ~T
at zo :
But then
by replacing h by
with c > 0sufficiently large,
we mayalways
achieve that
(zo)
has at least :n-~-1 positive eigenvalues.
PROOF. To prove Theorem 1 we have to show that
given f E (D),
with
af =
0 and s> n - p,
we can find a u E(D)
such thatWe may assume that
f
is the element we have chosen in n. 8b),
sothat
f’
=(D)
and-4~~&4~~ f’
= 0.Equation (1)
is thereforeequi-
valent to the
equation
wherein we want to show the existence of a solution u’ E