A NNALI DELLA
S CUOLA N ORMALE S UPERIORE DI P ISA Classe di Scienze
E DOARDO V ESENTINI
Remarks on integral inequalities on complex manifolds
Annali della Scuola Normale Superiore di Pisa, Classe di Scienze 3
esérie, tome 20, n
o3 (1966), p. 595-611
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ON COMPLEX MANIFOLDS (*)
EDOARDO VESENTINI
Let M be a connected orientable and oriented differentiable manifold of class
C°° ,
endowed with acomplete
riemannian metric. The action of theLaplace operator
11 on anyq-form u
of classC2
on M can beexpressed
lo-cally by
In this formula
Vi
and Vi stand for covariant derivatives withrespect
to the riemannian
connection,
and n is amapping
of the space of real va-lued
q-forms
intoitself,
which is linear over thering
of real continuousfunctions on M. The
operator x
issymmetric
withrespect
to the scalar pro-duct, (, )~ ,
definedby
the riemannian metric at eachpoint x
E M.Setting
we
call I u Ix
thelenght
of the form u at thepoint
x. We introduce also theL2 norm
-
ax
being
the volume element of the riemannian metric of M.The
following
theorem has beenproved
in[5] :
Pervenuto alla Redazione il 23 Febbraio 1966.
(*) Supported in part by the European Office of Aerospace Research under Grant
AF-EOAR, 65-42.
7. Annali dedla scuoda Norin. Sup.- Pisa.
THEOREM Let the
synunet1"ic ~x , acting
on the spaceof q-forms
onM,
bepositive semidefinite
a,t eachpoint
x E M outside acompact
K C M.
Any q-form 99 of
classC2
on suchthat 11
00,11 Llcp II
00 ,satisfies
theinequality
The
proof depends
on a~nintegral inequality estimating
theL2
norm11
VuII
of the covariant derivatives of aq-form
it in terms of11
duII, II
6u11
f8
and of the
integral
In this paper we extend the above theorem to vector bundle-valued
(p, q)-forms u
on acomplex
manifold.In the
proof
we establish anintegral inequality estima,ting
theL2
normof all the covariant derivatives of u in terms
of 11 au II, BI
Ou11
and of anintegral
oftype .f ( xu, u ) dX. A few direct applications
of that inequality
x
are listed in n. 8. The first section
(nn. 1-3)
contains somepreliminary properties
whoseproofs
can be found in[1]
or in[5].
§
1. -Preliminaries.
1. Let X be a
complex
manifold ofcomplex dimension n,
and letE -~ .X~
be a
holomorphic
vector bundle of rank m on X. be anopen coordinate
covering
of ~’ suchthat,
on eachUi, Ej
~~ isisomorphic
tothe trivial bundle. The bundle E is
defined,
withrespect
to thiscovering, by
asystem leijl
ofholomorphic
transition functionssatisfying
thecompatibility
conditionThe dual bundle E* of .E is defined on the
covering CJ1 by
thesystem
of
holomorpbic
transition functionsexpressed by
Let Cpq
(X, E)
be the vector space of continuous(p, q)-forms
with values in E.Any element cp
of Cpq(X, E)
is definedon Ui by
a continuous vectorvalued p, q).form q;
= ... ,gg-)
such thatA metric
along
the fibers of E is definedby
apositive
definite hermi- tian scalarproduct h (u, v) (u,
v E n-1(x),
x EX)
on the fibers of .Edepending differentiably
of class C°° on thepoint
x E X. If on the coordinateneigh-
bourhood
U ,
y then the local ex-pression
of h(u, v)
onUi
isgiven by
where
hi
is apositive
definite hermitian matrix of class C°° onThe metric Iz
along
the fibers of .E enables us to define an antiisomor-phism
which is
local,
i.e. preserves thesupports.
For anyform 99 = (ggi)
ofopq (X,
.Ewe have
2. The local forms
define a a-connection on
E,
and hence an absolute differentiation of any C’ section of E in thefollowing
way.The connection form 1 is
expressed,
in terms of a localcomplex
coor-dinates
system (z1,
... ,by
an m X m matrix of C°°(1, 0)-forms
A C’ section t of E is
locally represented by
an m-vector of class C’We define the covariant derivatives
of t, setting locally
Let 0 be the
holomorphic tangent
bundle on X. The vector~a~=i ~.a==i m? represents locally
aglobal
continuoussection, P’t,
ofthe
holomorphic
vector bundle .E@ @* .
Similarly represents locally
aglobal
continuoussection 17" t of the vector bundle 0, ’ .
The
conjugate 1 = I ij)
of the connection form 1 on .E defines a a- connection in theantiholomorphic
vector bundle E. If u is a 01 section ofE,
we define the covariant derivatives V’u and V"u in terms of the cova-riant derivatives of the section u of
E, setting
Using
the a - anda-connection
forms we can define covariant de- rivatives of 01 sections of tensorproducts
ofholomorphic
and antiholo-morphic
vector bundles.-
The metric h
on E,
considered as a C°° section of .E@ E,
has all itscovariant derivatives zero.
The curvature form of the a-conllection form 1 is
given locally by
a m X m matrix
of scalar C°°
(1, 1) forms
Letting
t be aC2
section ofE,
we have3. We assume now a C°° metric
along
the fibers of0.
This isequiva-
lent to
saying
that apositive
definite hermitian differential form of classC°° ~ gap
dzo. isassigned
on X. This form induces a C°°positive
definiteriemannian metric on the
underlying
C°° manifold of X. The *operator
definedby
the riemannian metric of X maps scalar(~, q)-forms
into scalar(n
- q, n -p)-forms,
and extendstrivially
to anisomorphism
The a-connection determined
by
the hermitian metric on X is a sym- metric connectionif,
andonly if,
the hermitian metric is a Kahler metric.In that case, the curvature form of the a-connection form coincides with the Riemannian curvature form of the
underlying
riemannian metric.Let qJ, 1jJ E
Cpq(X, E). Then qJ
A *#
1p is a scalar(n, n)-form.
If dXdenotes the volume element of the hermitian metric of
X, q
A *fip y
canbe written as
A
(q, acts,
at eachpoint
ofX,
as asesquilinear positive
definite hermitian scalarproduct
on the space Crq(X, E).
We set
and we
1
thelenght
of the form 99.Let
gpq (X, E)
be the space ofcompactly supported
C°°( p,
with values in .~.
The scalar
product
gives (X, E)
the structure of acomplex pre Hilbert
space overd.
LetE)
denote thecompletion
ofE)
withrespect
to the norm1
-
We denote
by JS
the formaladjoint
ofthe a operator,
i.e. the linearoperator
such that
Let us consider the scalar
product on ~
and let N be the norm defined
by
= a~).
We denote
by
Wpq(X, E)
the Hilbert spacecompletion
of(X, E)
with
respect
to the norm N.PROPOSITION 1
[1, 5].
-If
the hermitian metricof
X iscomplete,
Wpq(X, E)
can beidentified
with the spaceof
E(X, E)
which admit~c
(X, E)
and a E(X, E) (in
the senseof distribzctions).
Let us introduce the
Laplace-Beltrami operator R
=81S -~-
PROPOSITION 2
[1, 5].
-If
the metricof
X isc01nplete,
thenfor
any(p,
with values in E andof
classC2
onX,
andfor
anypositiroe
constant g, we haveCOROLLARY 3. - Under the same
hypotheses of proposition 2, if
, then g~ E
(X, E).
§
2. -Integral inequalities.
4. We suppose that the
complex
manifold X isequipped
with a(posi-
tive
definite, C°°)
hermitian metric. We choose also a metricalong
the fibersof the
holomorphic
vector bundle E.We denote
by
V’ and V" the covariant derivatives withrespect
to thegiven
metrics. We shall use the samesymbols V’
andV"
to denote cova-riant derivatives of sections of different bundles.
Let T
be a(p, q)-form
with values in.~,
of classC2
onX; 99
islocally represented by
a vector form of classC2
where A and B denote blocks
of p and q
indicescovariant derivatives
V’, V",
theoperator a
has theexpression
where
and
S~Y being
the torsion tensor of the connection.Analogously
we havewhere
Setting
where and
If the hermitian metric on X is a Kahler metric then S =--
0,
henceT =
0,
and thereforei
In
general
By
the Ricciidentity,
y the last summand of(1)
can beespressed by
where x is a hermitian
mapping
which is linear over the
ring J
ofcomplex
valued continuous functions on X and hermitian withrespect
to the scalarproduct A (, ).
Its localexpression
involves
linearly (with integral coefficients) only
the coefficients of the cur-vature forms of the metrics on .E and on X.
If q
=0,
then x = 0.A direct
computation yields
where ,,0
involvesonly
the curvature tensor of the hermitian metric on X.It has been shown in
[1] (see
also[5])
that there exist universalpositive
constants c~ , c2 such
that, if 99 ECppq (X, E),
thenIf the hermitian metric on X is a Kihler
metric,
then we can choosec2 = 1 ;
fur thermore with this choice the aboveinequality
becomesan
equality
5. We shall now establish an
integral inequality
on Xinvolving
boththe V’ and
P"
derivatives.We have
(consider
thetangent
vector field on Xwhere
An easy
computation
shows thatWe have
= gflm
By
the Ricciidentity
where
here x§
involvesonly
the curvature tensor of the hermitian metric of X.Let us introduce the
7--linear
hermitianoperator
We have
by (1)
and(3)
A direct
computation
shows thatwhere x2
involvesonly
the curvature tensor of the hermitian metric on X.Let the hermitian metric be a Kahler metric.
(X, E)
wehave
i,e,
by (5)
In the
general
case(i.e.
if the hermitian metric on X is notnecessarily Kahler),
we have for any 99 E(Dpq (X, E),
o
i.e.
We shall now estimate the last three summands on the
right
hand side.There exists a C°° function g
(x)
> 0 on X such thatthe
function g (x)
can be so chosen to involveonly
the torsion tensor and its first covariant derivatives.Repeating
the sameargument
for all terms-
of the
expression
ofD - D appearing
in(2)
and forI p 12,
we seethat there exist C°° functions
fi (x) ;~~ 0 (i = 1, 2, 3)
on X such thathence,
for any a > 0The
functions fi
can be so chosen to involveonly
the torsion tensor and its first covariant derivatives. When the hermitian metric on X is a Kahlermetric,
we may assumefi
==f2 --- f3
==E 0 on X.Setting
0 =1 ,
4 andwe can state the
following
PROPOSITION 4. -
Every
q E(X, E) satisfies
theinequality
If
the metric on X is a1netric,
then cpsatisfies equality (6).
6. We assume now that X satisfies the
following
condition :a)
There is acomplete
hermitian metric on X and acompact
setsuch that the hermitian form A
(x3
g,cp) acting
on the space Cp~(X, ~)
is
positive
semidefinite at eachpoint
of X - K.If follows from
proposition
4 that there exists a constant c h 0 suchthat,
for every 99 E(X, E),
whence, by Corollary 3,
LEMMA 5. -
If
Xsatisfies
conditionsa),
every(p, of
classC2
on
X,
with values inE, for
whichLet A = A
(t)
be a real C°° function on1R. Setting ,
we assume
that i (t)
>0~ ~ (t)
h 0 on1R,
and that(t) =
0 outside abounded interval of
1R.
.
1%
conditiona) is satisfied,
the
following inequality
holdsPROOF. Consider the
tangent
vectorfield ~
on Xlocally
definedby
We bave
...
Since
A, (t)
vanishes outside a boundedinterval, then A
is bounded on1R
by
a constant c1 > 0. On the other hand there exists apositive
constant C2 such thatbence
Furthermore
by (5)
Hence
by
with
Let es be a
positive
constant suchthat I (t)
= 0 when t>
c3 . We haveBy (8)
we haveThus, by
lemma5,
We conclude that
It follows from a theorem of M. P.
Gaffney [2]
that11
i.e.
Applying again (7) ~
we obtaininequality (9).
REMARK 1. - If the
complete
hermitian metric on X is a Kahler metric outside thecompact K, then x2
= x3 on K.Hence, by
lemma5,
inequality (9)
holds whenever ·2.
If q
hascompact support,
then for any choice of 1.Hence
inequality (9)
holds for(X, E)
and for all real C°° functions~ A
(t),
with~1 (t)
> 0.§
3. -Applications.
7. A MAXIMUM PRINOIPLE. THEOREM I. - Let X be a connected
complex manifold satisfying
thefollowing
condition.a) There exists a
complete
hermitian metric on X and ac01npact
set K c X such that the hermitianf orm
A(X3
99,acting
on Opq(X, E),
isposi-
tive
semidefinite
at eachpoint
K.Let (p
be a(p, q) form,
with values inE, of
classC2
o~zX,
such thatThen at each
point of
XPROOF. Let co =
Sup 1
onSupp (0
and suppose that co is finite. Let A = A(t)
be a real C°° function on1R
such thatoutside a bounded interval.
The
right
hand side of(9) vanishes,
while the left hand sideyields
Let I > c,,
at somepoint
of X,Since ~ (t) >
0 for t> co,
y it follows from the aboveinequality
that =0,
p" g =0,
io aneighbourhood
ofthat
point.
Hence11
=0, |Q|2
= 0 andtherefore I qJ (2
is constantin that
neigbbourhood.
But this isabsurd,
since .X is connectedis continuous on X.
Q.E.D.
In view of remark 1 of n.
6~
if the hermitian metric of X is a Kabler metric on X - K then condition("2
~~)
oo may bedropped.
HenceTHEOREM I’. -- Under the same
hypotheses of
theorem I andif
more the
complete
hermitian metric on .X is a, Kdhler metric on X -K,
ine-quality (11) holds, provided
that1199 II
00,II II
00 .8. If .g = z and if the hermitian metric on X is a
complete
Kahlermetric,
the results of n. 7 can besharpened.
The mostinteresting
result inthis direction concerns the case of a square summable
holomorphic
sectionof E.
Let X be a
complete
connected Kahler manifold. Assume a metricalong
the fibers of .E and consider the
corresponding
curvature formPROPOSITION 8. -
If
the hermitianform
is
positive semidefinite ( possibly
=--0)
at eachpoint of
X then every holont014-phic
section 1pof
E such thatII
yII
oo has constantlenght
on X.If
theform (12)
ispositive definite
at somepoint of X,
orif
X hasin,finite
volume(with respect
to the Kählermet,,"ic), then 1p
== 0.PROOF. The metric on X
being
a Kahlermetric,
a directcomputation
showsthat,
for every 99 E C°°(X, .E),
Since this hermitian form is
positive semidefinite, proposition
4yields :
for every q; E
CDOO (X, E).
Henceevery 99 c
Woo(X, .E )
of class01
admits co-variant derivatives . , V" p. - . such
that 11
I .. I I .. Further-more such a g satisfies
(13).
"
The
form V
is oftype (0, 0)
andholomorphic.
Thuswhence
(Proposition 1) : 1p E
Woo(X, E).
It follows from(13),
thatV’1jJ
=0, V" 1p
=0,
andtherefore I
is constant 0 if vol X = 00. If(12)
is
positive
definite at somepoint
ofX, then y
== 0(in
aneighbourhood
ofthat
point
andtherefore)
on the whole manifold X.Q.E.D.
An immediate consequence of
proposition
8 is thefollowing
COROLLARY 9. - Under the
hypotheses of Proposition
8 the spaceof
square
integrable holomorphic
sectionsof
.E hasfinite
dimensiond,
withd m = rank E
if
Vol(X )
oo, d = 0 otherwise.If .E is the trivial
bundle,
and if the trivial metric is chosen onit, (12)
vanishes
identically
on X.Proposition
8yields :
If a holomorphic function
on the connected1nanifold
X is square ble withrespect
to acomplete
Kählermetric,
then thefunction
is constant onX, equal
zeroif
the volumeof
X isinfinite.
Let E be the
holomorphic
vector bundle of C°°(~, 0)-forms (with
scalarvalues),
and assume on E the metric inducedby
the Kahler metric of X.The hermitian form
(12) becomes, apart
from an inessentialpositive
cons-tant
factor,
B - being
the Ricci tensor of X. If(14)
ispositive
semidefinite at eachpoint
of X all square summableholomorphic p-forms
on X have constantlenght
on X.The space
spanned by
these forms has finitedimension,
which is zeroif Vol
(X) .
= oo , or-,-n (P) if Vol (X)
oo . The extreme vale B-P/ is at-
tained,
foristance,
when X is acomplex
torus.If p = n, .E can be identified with the canonical bundle on X. The metric induced on E
by
the Kahler metric on X is definedlocally by
thefunction
(det
In view of thischoice,
we have thatThus the fact that a form is square
integrable
isindependent
of thechoice of the metric on X
[4].
The hermitian form(14) becomes, apart
froman inessential
positive
constantfactor,
R
being
the riemannian curvature of X.Hence :
If
the connectedcoinplete
Kählcrmanifold
X has riemannian curvature R > 0everywhere
onX,
then every square sumtnableholomorphic (n, 0)
on, X has constant
lenght
on X.If R )
0 at somepoint of X,
orif Vol (X)
= cxJ,= 0.
REFERENCES
[1]
A. ANDREOTTI - E. VESENTINI, Carleman estimates for the Laplace-Belframi equatin on complex manifolds, Publications Mathématiques de l’Institut des Hautes Études Scientifiques, n° 25 (1965), 81-130; Erraturn, ibd. n° 27, 153-155.[2]
M. P. GAFFNEY, A special Stokes’s theorem for complete riemannian manifolds, Ann. of Math., 60 (1954), 140-145.[3]
L. HÖRMANDER, L2 estimates and existence theorems for the 03B4-operator, Acta Mathematica 113 (1965), 89-152.[4] S. KOBAYASHI, Geometry of bounded domains, Trans. Amer. Math. Soc., 92 (1959), 267-
290.
[5]
E. VESENTINI, Levi convexity of complex manifolds and cohomology vanishing theoremsLecture notes, Tata Institute of fundamental Research (to appear).
Istituto Matematico Univer8ità di Pisa