C OMPOSITIO M ATHEMATICA
P AOLO DE B ARTOLOMEIS
G IUSEPPE T OMASSINI
Traces of pluriharmonic functions
Compositio Mathematica, tome 44, n
o1-3 (1981), p. 29-39
<http://www.numdam.org/item?id=CM_1981__44_1-3_29_0>
© Foundation Compositio Mathematica, 1981, tous droits réservés.
L’accès aux archives de la revue « Compositio Mathematica » (http:
//http://www.compositio.nl/) implique l’accord avec les conditions gé- nérales d’utilisation (http://www.numdam.org/conditions). Toute utilisa- tion commerciale ou impression systématique est constitutive d’une in- fraction pénale. Toute copie ou impression de ce fichier doit conte- nir la présente mention de copyright.
Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques
http://www.numdam.org/
29
TRACES OF PLURIHARMONIC FUNCTIONS
Paolo de Bartolomeis and
Giuseppe
Tomassini@ 1981 Sijthoff & Noordhoff International Publishers - Alphen aan den Rijn
Printed in the Netherlands
Introduction
Let M be a real oriented
hypersurface
in acomplex
manif oldX,
which divides X into two open sets X+ and X -.In this paper we characterize in terms of
tangential
linear diff eren- tial operators on M the distributions T on M which are"jumps"
ortraces
(in
the sense ofcurrents)
ofpluriharmonic
functions in X+ and X -.The
starting point
of ourinvestigation
is thenon-tangential
charac-terizing equation ~b~T
=0,
which can be deduced from thetheory
ofboundary
values ofholomorphic
forms. If M is notLevi-flat,
weconstruct a second order
tangential
local linear differential operatorwM such that if T is the trace on M of a
pluriharmonic
functionh,
thenCùM(T)
= ah. This enables us to prove that thetangential equation
abC»M(T)
= 0 characterizeslocally
the traces on M ofpluriharmonic
functions on X+ or X -
(local Cauchy-Dirichlet problem).
From thislocal result we deduce
directly
theglobal solvability
of theCauchy-
Dirichlet
problem
in the case M is either compact or its Levi form haseverywhere
at least onepositive eigenvalue.
Finally, using
standardcohomological
arguments theglobal
Rie-mann-Hilbert
problem ("jumps"
ofpluriharmonic
functions onXBM)
is solved if
H2(X, C) = 0
orH’(M, R)
= 0. Particular cases of ourproblem
have beeninvestigated
in[1], [3] (cf.
also[2], [4]).
The present paper contains an
improved
version of the results announced in[5].
1. Preliminaries and notations
In the present paper X will be a
complex
manifold of dimensionn 2:
2,
and M C X a real oriented connected C°°hypersurface.
0010-437X/81107029-11$00.20/0
We assume M is defined
by
p = 0 where p : X ~ R is a C°° function such thatd03C1 ~
0 on M.We say that such a p is a
defining function
forM ;
M divides X into two open sets X+ andX -,
definedrespectively by p > 0
andp
0;
if U is an open subset ofX,
we will set U± = U flx±;
we canalso assume that there exists an ~0 > 0 such that
if JE
Eo andMe
isthe level
hypersurface
definedby
p = e, there exists adiffeomorphism
03C0~: M~~M.
We will use the standard notations for currents and distributions spaces
(cf.
e.g.[9]);
inparticular
we fix the orientation on M in such away that
d[X+]
=[M].
Furthermore we list the
following
definitions:i)
Let L:(r)(X) ~ (r)(M)
be the restriction operator; we set:(p,q)(M)
=L((p,q)(X)).
ii)
Let K E2(’)(M):
K A[M]
will be the(r
+1 )-current
on X definedby: (K
A[M], ~)
=(K, L(~)>, ~
Egy(2n-r-1)(X).
iii)
We say that K E2’(")(M)
is a(r, 0)-current (resp. (0, r)-current)
if(K
A[M])P,q
= 0 for p :5 r(resp. (K
A[M])q,p
= 0 for p :5r);
we denoteby 2’(10)(M) (resp. D’(0,r)(M))
the space of(r, 0)-currents (resp. (0, r)- currents).
iv)
If K E2’(ro)(M),
then K A[M]1,0
is the(r
+1, 0)-current
definedby: (K
A[M]’’°, ~) = (K, L(cp)), cp
ED(n-r-1,n)(X)
and K A[M]0,1
is the(r, 1)-current
definedby: (K
A[MI’,’, ~> = (K, L(cp»
cp E9)(n-r, n-1)(X).
v)
Let a Ec¡g(2)(X+);
we say that a admits trace K E2’(")(M)
on M inthe sense of currents if for every cp
~ D(2n-r-1)(M)
we have:(cf. [8]);
we set K =y+(a);
in the same manner we definey-(a)
if03B1 ~
(r)(X-).
Let a E
e(’)(XBM)
such thaty+(a)
andy-(a)
exist: we refer to03B3+(03B1) - y-(a)
as thejump
of a on M.We denote
by (r,s)*(X±)
the space of forms a E(r,s)(X±)
such that03B3~(03B1)
andy±(da )
exist.Observe that if a
~(r,0)*(X+),
inparticular
we have2.
Tangential
operators on M2a)
The smooth caseA local linear operator 03A6:
(p,q)(X) ~ (r,s)(M)
is said to be tangen- tial on M if fromL(f )
= 0 it follows03A6(f)
=0;
atangential
operator induces a new operator:(p,q)(M) ~ (r,s)(M)
which will be denotedagain by
03A6.Let now
(,)
be a Hermitian structure onX;
without loss ofgenerality
we can assume(ap, ap) = 2
on M. Define:We have the
decompositions:
1
and we denote
by:
the natural
projections;
observe thatT(a) = T(¡3)
isequivalent
to03B1 039B [M]1,0 = 03B2 039B [M]10;
we set ~b = 03C4 03BF L 03BF ~ and~b = 03C4 03BF L 03BF ~;
by definition ab
andib
aretangential
operators on M(cf. [6]).
The induced operators
are described
by
the formulasThus
We consider in
particular
thefollowing
cases:f
E(0,0)(X)
and03B2
E(1,0)(X).
a) if
f
E(0,0)(X)
set:so we obtain on M:
furthermore it is easy to check that:
i)
at everypoint
of M,N(f)
represents thecomplex
normal derivativeof f
andN(f) + N(f)
is the real normal derivative off.
ii) f
HN(f) - N(f)
is atangential
operator onM ;
thus we have alsoe.g. : .
b) if 0
E(1,0)(X)
defineN1(03B2)
andN1(03B2) by
the relations:we observe that
(3 t---+ N1(03B2) - N1(03B2)
is atangential
operator, and sowe obtain on M the
decomposition:
which
again
enables us to isolate thegenuine non-tangential
com- ponent ofL(~03B2), namely (N1(03B2) + N1(03B2))
039BL(ap).
Let U ~ X be an open set and
let 9P(U)
be the space of realpluriharmonic
functions on U(i.e. f
EP(U)
ifff
is real valued andaaf
=0).
We have the
following:
PROPOSITION 2.1: Assume
L(ap
A ap A~~03C1) ~ 0;
then there exists alocal linear
differential
operator R :(0,0)(M) ~ (0,0)(M)
such thatif
h E
P(X)
thenR(L(h))
=L(N(h)
+N(h)).
PROOF: Let h
E 9P(X):
define Sb = ab + ab,*03B4b
= Tab + Tab,S b
=i(~b - ab);
thenomitting
L tosimplify
our notations:and also
thus we obtain the relation:
taking
the Hermitianproduct,
we have:Since
i03C4(~b~03C1),
which is a real operator, represents the restriction to M of the Levi form of p, in ourassumption ~i03C4(~b~03C1)~2 >
0everywhere
and so the R we are
looking
for isgiven by:
We observe that in
[10]
a similar formula isproved
in a morelaborious way.
For
example
in the case X =B2,
the unit ball inC’,
and M =b B2,
weobtain the formula:
(cf. also [1]).
Proposition
2.1 shows that if h is apluriharmonic
function on Xand M is not Levi-flat
anywhere,
then the real normal derivative of hon M can be
expressed by
means of a realtangential
operator R.Thus we have on M:
let Cl)M :
(0,0)(M)
-(1,0)(M)
be definedby
theright
member of(*)
wehave the
following:
REMARKS 2.2:
a) if f ~(0,0)(M),
then~b03C9M(f)
= 0.(b) if f
is the restriction of apluriharmonic
function F then~b03C9M(f) =
0.
PROOF:
a)
Letf E (0,0)(X+)
be an extension off ; by
Stokes’theorem, L(ap)
A[M]1,0
=0,
soCl)M(f)
A[M]1,0
=abf
A[M]1,0
=~(f[M]1,0)
and therefore~03C9M(f)
A[M]1,0 = 0,
so~b03C9M(f)
= 0.b) By (*), wm(f)
=L(aF)
soCl)M(f)
A[M]0,1 =
aF A[M]O,’.
Since F ispluriharmonic, ~(03C9M(f)
039B[M]O,’)
= 0 and therefore~b03C9M(f)
= 0.2b)
Extension to thegeneral
case.Consider the dual
decompositions:
where the
projections
T and r are defined in an obvious way, so the operators ab andab
extendnaturally
to currents on M. Furthermore it turns out that Ni andNi
are defined asN1, N1: 1,0*(X±) ~ D’(1,0)(M)
and
they
induce a continuous operatorNi-N1: gy10,O)(M)
-D’(1,0)(M);
so if
e.g. 0 ~(1,0)*(X+)
we have:Of course
~03B2 = 0 implies N1(03B2) = 0;
we note also thatif p
isholomorphic
or(3
=a f
for a real valuedf,
thenN1(03B2)
=0;
inparti-
cular if
03B3+(03B2)
=03B3+(f)~03C1
for a real valued functionf,
then:Finally
we have that MM can be extended as an operatorWM :
D’(0,0)(M)
~D’(1,0)(M) and
remarks 2.2a), b)
hold.3. Traces of
pluriharmonic
functionsWe are able now to
give
thefollowing
local solution to the traceproblem (Cauchy-Dirichlet problem)
for theaa
operator.THEOREM 3.1: Let p E M and U be a
neighbourhood of
p ; assumeL(ap
A03B403C1
A~~03C1) ~
0 on M ~ U and let T be a real distributiondefined
on U rl
M ;
then thefollowing
statements areequivalent : i) ~b03C9M(T) = 0
on Un Mii)
there exists aneighbourhood
Vof
p and there exists F EP(VBM)
such that03B3+(F) - 03B3-(F)
= T in U ~ V ~M;
moreprecisely if
the Levi
form of
p has apositive (resp. negative) eigenvalue
at p wecan choose
F 1 v-
= 0(resp. F|V+
=0)
and so T isactually
the traceof
a
pluriharmonic function.
PROOF: We have
already
observed thatii) implies i); conversely
assume
~b03C9M(T)
= 0 on U nM ;
let W C U be a Steinneighbourhood
of p:
by assumption
wehave: a [wm(T)
A[M
nW]0,1]
= 0 in W and sothere exists
K
Egyf(1,O)(W)
such that~K
=wM(T)
A[M
nW]0,1.
|w+
and|w-
areholomorphic (1, 0)-forms
in W+ and W- respec-tively, |w±~(1,0)*(W±)
and03B3+(|w+) - 03B3-(|w-) = 03C9M(T)
on M n W(cf. [8]
th.II1.3).
Now assume the Levi form of p has e.g. apositive eigenvalue
at p; thenklw-
extends across M as aholomorphic (1,0)-
form
03B2
to a Steinneighbourhood
V of p: if K+ =k 1 v,
of course wehave:
03B3+(K+ - 03B2)
=lùM(T)
on M ~ W.Furthermore we have:
in fact
N,(K+ - 03B2)
= 0 and so:Let now
(fn)n~N
be a sequence of elements of(0,0)(V)
such thatL(fn) ~
T inD’(0,0)(M
~V);
from(°)
it followswhich proves
(**).
Now in V we have:
and thus
~(K+-03B2)039B[V+]
isholomorphic
in V and so~(K+- 03B2) ~ 0
on V+.It follows that on V:
a [(K+ - j8)
A[V+] -
T 039B[M
rlV]1,0]
= 0 and soit is
possible
to findÔ
ED’(0,0)(V)
such that:Then if we set G =
GBVBM
we obtainaao
= 0.Thus we have the
following:
a)
G is apluriharmonic
function inVBM
b)
Since G can be extended as a distribution across M and satisfiesaaG
=0,
then(cf. again [8]
corollaire1, 2.6.) y+(G)
andy-(G)
exist.
c)
On V+ one has aG = K+ -0.
We have also that
03B3+(G)
+ T isab-closed:
in fact:Thus there exists an
antiholomorphic
function H on V+ such that-y,(H) = 03B3+(G)
+ T.It follows that F = H - G is a
pluriharmonic
function on V+ such thaty+(F)
= T and since T is real weactually
havey+(Re F)
= T and theproof
of Theorem 3.1. iscomplete.
From Theorem 3.1. we can deduce first the
following global
solu-tions of the
Cauchy-Dirichlet problem:
PROPOSITION 3.2:
Suppose
the Leviform of
p has least onepositive eigenvalue
at everypoint
p E M. Then there exists aneighbourhood
Uof
M such that theequation ~b03C9M(T)
= 0 characterizes those dis- tributions on M which are tracesof pluriharmonic functions
in U+.PROOF: Theorem 3.1. assures that there exists a
covering
U =(Un)n~N
of Mby
open set of X such that for every n E N thereexists
f n
EP(U+n)
for which03B3+(fn)
= T on M rlUn ; furthermore,
ifUn fl Um rl M ~
0,
one has03B3+(fm)
=03B3+(fn)
on Um ~ Un rl M andthus,
since the trace on M characterizes apluriharmonic function,
we havefm = fn
onU+n ~ U+m
etc...PROPOSITION 3.3:
Suppose
X is a Steinmanifold,
X+ isrelatively
compact andL(ap
Aap
A~~03C1) ~
0.If
T is a real distribution onM,
then thefollowing
statements areequivalent :
PROOF:
i)
followsimmediately
fromii);
assume nowi)
holds: in order to proveii),
we argue in the same way as in Theorem3.1, setting
W = X andusing Hartog’s
theorem to extendKlx-
to thewhole X.
Using
standardcohomological
arguments we caninvestigate
theglobal
Riemann-Hilbertproblem.
Let Y be the sheaf of germs of real distributions T on M such that
~b03C9M(T)
= 0 and letY
be its trivial extension to X. Let s4 be the sheaf of germs of distributions T on M such that~bT
= 0.Furthermore,
let ex be the sheaf of germs of realpluriharmonic
functions on X and*PM
the sheaf on X associated to the canonicalpresheaf:
Assume
L(ap
039B~03C1
039Baap) Y-4
0 on M.Let Re: A ~ J be the sheaf
homomorphism
definedby
T - real part ofT,
and let a be the sheafhomomorphism
definedby:
03B1:*PM ~ J
COROLLARY 3.4: The sequences
are exact.
PROOF: We need the
following
LEMMA 3.5:
Suppose
M is notLevi-flat
at p and let U be aneighbourhood of
p; letf± ~ P(U±) admitting
traces-y,(f,)
and03B3-(f-)
on U ~M.If furthermore 03B3+(f+)
=03B3-(f-),
then there existsf ~ P(U)
such thatf 1 u±
=f±.
PROOF OF LEMMA 3.5: Since the
problem
islocal,
we can assume U is a domain of Cn : then~f± ~zj, 1 ~ j ~
n, areholomorphic
inU±, -y, af+
and
03B3-(~f- ~zj)
exist andProposition
2.1. assures that03B3+(~f+ ~zj) = 03B3-(~f- ~zj),
1
S j S n ; hence,
we areessentially
reduced to the casef ±
holomor-phic
which follows from[8],
Corollaire II 1.2.PROOF OF THE COROLLARY 3.4:
(1)
In virtue of Theorem 3.1. a issurjective
and theprevious
lemma concludes theproof
of the exact-ness of
(1).
(2)
As a consequence of Lemma3.5,
we deduceeasily
thatker Re =
lm(î)
and so we have to check that if p E M and T EYp
then there exists
f
EAp
such that ReT
= T.Now in virtue of Theorem
3.1,
there exist aneighbourhood
U of pin X and F E
P(UBM)
such that: T =03B3+(F) - 03B3-(F);
from[8]
wededuce that there exists G E
O(UBM)
such that Re G = F andy+(G), 03B3-(G) exist; (more
in detailthe,argument
runs as follows: holomor-phic
andpluriharmonic
functions with traces in the sense of currentsare characterized
by
finite order ofgrowth
with respect to p([8]
Corollaire
1 2.6.)
so F has finite order ofgrowth
with respect to p andso does
G,
which can beexpressed locally
as G = F +iH,
where Hsatisfies dH = d’F
etc ...);
it follows that Re: A ~ J issurjective
and(2)
is exact: so theproof
ofCorollary
3.4 iscomplete.
THEOREM 3.6:
(Global
solutionof
the Riemann-Hilbertproblem for aa) Suppose
X is a Steinmanifold
andL(ap
039Bap
A~~03C1) ~ 0;
assumefurthermore H2(X, )
= 0 orH’(M, R)
=0;
thenif
T is a real dis-tribution on
M,
thefollowing
statements areequivalent : i) ~b03C9M(T)
= 0ii)
there exists F EP(XBM)
such that03B3+(F) - 03B3-(F)
= T.PROOF: We observe that for a Stein manifold X we have the
isomorphism Hr(X, PX) ~ Hr+1(X, C)
for r ~1;
moreover we have:H O(X, ) ~ H’(M, J).
If
H2(X, C)
= 0 we obtain the exact sequence:If
H1(M, R)
= 0 we obtain the exact sequence:This concludes the
proof.
REFERENCES
[1] T. AUDIBERT: Caractérisation locale par des opérateurs differentiels des restric- tions à la sphère de Cn des fonctions pluriharmoniques C.R.A.S. (1977) A284
1029-1031.
[2] E. BEDFORD:
(~~)b
and the real part of CR functions Indiana Univ. Math. J.(1980) 29 3 333-340.
[3] E. BEDFORD, P. FEDERBUSH: Pluriharmonic boundary values Tohoku Math.
(1974) 26 505-511.
[4] V. BELOSAPKA: Functions pluriharmonic on manifolds Math. U.S.S.R. Isvestija (1978) 12 439-447.
[5] P. de BARTOLOMEIS, G. TOMASSINI: Traces of pluriharmonic functions Analytic
Functions Kozubnik 1979 Lecture Notes in Math. 798 Springer (1980) 10-17.
[6] J.J. KOHN, U. ROSSI: On the extension of holomorphic functions from the boundary of a complex manifold Ann. of Math. (1965) 81 451-473.
[7] G. LAVILLE: Fonctions pluriharmoniques et solution fondamentale d’un opérateur du 4e ordre Bull. Sc. Math. 2s. (1977) 101 305-317.
[8] S. LOJASIEWICZ, G. TOMASSINI: Valeurs au bord des formes holomorphes
Several Complex Variables, Proceedings of International Conferences, Cortona Italy 1976-1977 222-245 Scuola Normale Superiore, Pisa (1978).
[9] J. POLKING, R. O. WELLS: Boundary values of Dolbeault Cohomology classes
and a generalized Bochner-Hartogs Theorem Abh. Math. Sem. Univ. Hamburg (1978) 47 3-24.
[10] G.B. RIZZA: Dirichlet problem for n-harmonic functions and related geometrical properties Math. Ann. Bd. (1955) 130 s.202-218.
(Oblatum 6-111-1981 & 5-VI-1981) Giuseppe Tomassini
Universitâ delqe Studi Istituto Matematico Ulisse Dine
Viale Morgagni 67-A
Firenze 50134
Italy