C OMPOSITIO M ATHEMATICA
K AZUMI T SUKADA
Holomorphic forms and holomorphic vector fields on compact generalized Hopf manifolds
Compositio Mathematica, tome 93, n
o1 (1994), p. 1-22
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Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques
http://www.numdam.org/
Holomorphic forms and holomorphic
vectorfields
oncompact generalized Hopf manifolds
KAZUMI TSUKADA
Department of Mathematics, Ochanomizu University, Tokyo 112, Japan Received 17 March 1992; accepted in revised form 20 June 1993
© 1994 Kluwer Academic Publishers. Printed the Netherlands.
1. Introduction
Let M be an
n( > 2)-dimensional
Hermitian manifold with metric tensor g andcomplex
structure tensor J. Forsimplicity,
all manifolds in this paperare assumed to be connected. If each
point p E M
has an openneighbor-
hood U with a differentiable function Ju : U --+ R such that
?lu
=e-’ug
is a Kàhler metric onU, g
is called alocally conformal
Kahler(l.c.K.)
metricand M is called an l.c.K.
manifold ([7]).
If we can take U = M, the metricg is called a
globally conformal
Kahler(g.c.K.)
metric and the manifold Mis called a
g.c.K. manifold.
If g is an Lc.K.metric,
it iseasily
shown thatduu
=duv
on U n V. Therefore the closed 1-form w(to
=duu
onU)
isdefined
globally
on M and is called theLee form
of an Lc.K. manifold M.The Lee form eo determines the first de Rham
cohomology
class[w]EH1(M;R).
If the metric g ischanged
tog’ = eag by
a differentiable function u onM, g’
is also an l.c.K. metric and its Lee form m’ isgiven by
to’ = ro + du. In
particular
we have[ro]
=[m’]
inH 1 (M ; R).
It follows thatg is
g.c.K.
if andonly
if[co]
= 0.Typical examples
of l.c.K.(and
notg.c.K.)
manifolds are theHopf
manifolds
Mex.
We setMex
= Cn _{O}/Ga
wherea E C,
0lai
1 andGx
isthe group
generated by
theholomorphic automorphism
z - az, z E Cn -{O}.
Then
Mx
is a compactcomplex
manifold. On cn -{O},
we consider the Hermitianmetric g
=1/11 z Il ’ Y-!= 1 dzi dzi
which isconformally
related to theflat Kàhler metric
Y-!. 1
dzi dzi. Themetric g
is invariant under the action ofGex
and induces a Hermitian metric onM03B1.
ThenMex with g
is an l.c.K.manifold.
It is an
interesting
and remarkable fact that compact l.c.K.(and
notg.c.K.)
manifolds admit no Kàhler metrics([9]
Thm.2.1).
Hence the classof compact
complex
manifoldsadmitting
l.c.K. metrics isessentially
differ-ent from that of Kàhler manifolds. We are interested in
topological
andcomplex analytic properties
of compact l.c.K. manifolds. Since not much has been known aboutthem,
we first focus ourstudy
on aspecial
class ofl.c.K.
manifolds, i.e.,
thegeneralized Hopf (g.H.) manifolds. By definition,
ag.H.
manifold is an l.c.K. manifold whose Lee form cv isparallel, i.e.,
Vu = 0
«(V
=1=0)
with respect to the Riemannian connection V of its Hermitianmctric g ([10]).
The class ofg.H.
manifolds contains theHopf
manifolds
Mx with g
mentioned above. Thetopology
of compactgeneral-
ized
Hopf
manifolds has beeninvestigated by
Kashiwada([4])
andVaisman
([10]).
Inparticular,
some remarkableproperties
about Betti numbers are known(Corollary
2.4 in thispaper).
In this paper we shall
study holomorphic
forms andholomorphic
vectorfields on compact
g.H.
manifolds. In Section 3 we deal with harmonic forms of thecomplex Laplacian
D and show that anyholomorphic
form isclosed
(Theorem 3.3).
Moreover we obtain thedecomposition br(M) - Lp+q=rhP,q(M)
for the Betti numbers(Theorem 3.5).
In Section4,
weinvestigate holomorphic
vector fields and obtain ananalogous
result to atheorem of Matsushima and Lichnerowicz
(Theorem 4.6).
In Section5,
we consider thefollowing problem:
What domain inH1(M; R)
isoccupied by
the Lee forms of all Lc.K. metrics on M?
(Theorem 5.1).
In Section 2 wereview basic
properties
of Kàhler foliations which are thekey
to ourstudy.
The author would like to express his thanks to the referee for his valuable comments.
2. Kàhler foliations and the
décomposition
of harmonic forms on a compactg.H.
manifoldIn this
section,
we shall show that a foliation iFcanonically
defined on ag.H.
manifold istransversally
Kàhlerian. We reviewproperties
of the basiccohomology
of Kâhler foliations and results about the Betti numbers of acompact
g.H.
manifold obtainedby
Kashiwada([4])
and Vaisman([10]).
Let
(M, g, J)
be an Lc.K. manifold with Lee form co. We denoteby (D
thefundamental form defined
by (D(X, Y)
=g (JX, Y).
We set 0 = -woJ anddenote
by B
and A the dual vector fieldscorresponding
to w and0, respectively.
Then we have A = JB.Computing
the Riemannian connec-tion V
of the local Kâhler metric?lu
=e-eug,
we getSince J is
parallel
with respect toV,
thefollowing
holds:From now on we assume that
(M,
g,J)
is ag.H.
manifold.By
a homotheticchange
of themetric g,
we may assumeIlwll I)
= 1. Since w isparallel,
B isalso
parallel. Putting
Y = B in(2.2),
we haveFrom these
equations,
we obtain thefollowing (for
dctailcd computa- tions see[8]).
LEMMA 2.1
(cf. [8]).
On ag.H. manifold (M,
g,J), the following
holds:(1) A
and B areKilling vector fields,
i.e.,LAg
= 0 andLB9
=0,
where Ldenotes the Lie derivative.
(2) A
and B areinfinitesimal automorphisms of (M, J),
i.e.,LAJ
= 0 andLBJ
= 0. Inparticular,
V = B -V// 1
A is aholomorphic vector field
on M.(3)
We haveVA A = VA B
=VBA
=VB B
= 0 and inparticular [A, B]
= 0.By
Lemma2.1(3),
the distributiongenerated by
the vector fields A andB is
completely integrable
and defines a foliation àF whose leaves are1-dimensional
complex
submanifolds. Moreover these leaves aretotally geodesic
andlocally
flat submanifolds of M. The foliation !F will be called the canonicalfoliation
of ag.H.
manifoldM,
which is called the verticalfoliation
in[10].
We shall show that f istransversally
Kahlerian.We review basic definitions and
properties
of the transversal geometry of foliations. For ageneral reference,
see Tondeur([6]).
Let ff be a foliationon a manifold M.
By
the transversal geometry, we mean "the differentialgeometry"
of the leaf spaceMIg;.
It isgiven by
an exact sequence of vectorbundles
where L is the tangent bundle and
Q
the normal bundle of F. We denoteby
I-’L andrQ
the spaces of differentiable sections of L andQ, respecively.
The action of the Lie
algebra
rL onrQ
is definedby LXS
=n[X, YS]
forany
XerL, s E TQ,
where5g G rTM
withn(Ys)
= s. This action is extendedto tensor fields of
Q.
A tensorfield ç
ofQ
is said to beholonomy
invariantif it satisfies
LxqJ
= 0 for any X c- FL. 3F is called aRiemannian foliation
ifthere exists a
holonomy
invariant Riemannian metric gQ onQ.
Ametric g
on M is bundle-like if the induced metric gQ on
Q
isholonomy
invariant. It is known that there is aunique
metric and torsion-free connection V’ inQ
for the Riemannian foliation àF with
holonomy
invariant metric gQ(cf. [6]
Thm.
5.12).
Inparticular,
for theholonomy
invariant metric gQ inducedby
the bundle-like
metric g,
such aunique
connection V’ isgiven by
where YS E
r L 1. withn( ys)
= .s. Here we denoteby
L-1 the vector bundle oforthogonal complements
of L in TM.A foliation F is
transversally
Kahlerian(cf.
Nishikawa and Tondeur[5])
if it satisfies the
following
conditions:(i)
F is Riemannian with aholonomy
invariant metric gQ onQ, (ii)
there is aholonomy
invariant almostcomplex
structureJQ
ofQ,
withrespect to
which gQ
isHermitian,
i.e.gQ(J QS’ JQt)
=gQ(s, t)
for s, t E1-Q,
and
(iii) JQ
isparallel
with respect to theunique
metric and torsion-free connection V’ associated with gQ.Returning
tog.H. manifolds,
we recall thefollowing,
which isimplicitly proved
as Theorem 3.1 in[10].
THEOREM 2.2. The canonical
foliation
57 on ag.H. manifold
M isKâhlerian.
Proof. Identifying
L 1. withQ,
we get an almostcomplex
structureJQ
andits Hermitian metric gQ on
Q. By
Lemma2.1(1)
and(2),
it is easy to see thatJQ and gQ
areholonomy
invariant andhence 9
is a bundle-like metric.We show that it satisfies the third condition of Kàhler foliations. For X E
FL, V’xJ Q
= 0 holds. In fact this means theholonomy
invariance ofJQ.
For X c- rL’ and s e
FQ,
we havewhere
YS E rL1.
withn(Ys)
= s.Now we return
again
to ageneral
foliated manifold M with codimension q foliation F. A differentialform il
ES2r(M)
is said to be basic if1(X)q =
0and
Lxq
= 0 for all X E r’L. The exterior derivative d preserves basic forms and the setS2B
=f2*(F)
of all basic forms constitutes asubcomplex
of thede Rham
complex (Q*(M), d).
We denotedlnB
=dB.
Itscohomology H*B(F)
is called the basic
cohomology
of F([6] Chap. 9).
From now on we assume that the manifold M is compact and
oriented,
and tl1at :F is
transvcrsally
oricntcd and Ricmannian with a bundlc-like mctric g. Morcovcr it is assumcd that F isharmonic,
i.c. ail ]caves of .3z7arc minimal submanifolds of
(M, N).
We dcnotc
by ÔB
the formaladjoint
opcrator ofdB
with respect to the natural scalarproduct , >B
inQB(F).
We put the basicLaplacian AB
=dBôB
+¿jBdB
and call a basicform il satisfying ABI
= 0 a harmonic basicform ([6] Chap. 12).
It is known that the spaceHrB
of harmonic basic r-forms is of finite dimension and thatHr B
isisomorphic
toHrB(F) (cf. [2]).
Furthermore suppose that iF is
transversally
Kâhlerian with codimen-sion q
= 2m. The fundamental 2-form 1>’ of a Kàhler foliation is definedby (D’(X, Y)
=gQ(J QnX, nY)
forX,
Y E rTM. Then (D’is a closed basic 2-form.The
complexified
normal bundleQ’
=Q (D, C has
the direct sum decom-position :
where
Q+
andQ -
are subbundles associated witheigenvalues /2013 1
and2013/20131 of JQ, respectively. According
to thisdecomposition,
thecomplex
valued basic r-forms
QrB(F)
aredecomposed
as follows:where
QsB(F)
denotes the space of basic forms of type(s, t).
The exteriorderivative d B: n(F) --+ nB " ’ ’ (F)
isdecomposed
into two operatorsOB
andôB
ofbidegrees (1, 0)
and(0, 1).
Then thefollowing
differentialcomplex
isobtained:
and its
cohomology Hs,tB‘(F)
is called the basic Dolbeaultcohomology
of ffi’.Let
3B
be theadjoint
operator ofaB
with respectto , >B.
We putDB = aB3B + 3BaB and
It is known that
Hs,tBt
is of finite dimension and thatHs,tB HBt(F)
andHBs,t = HBS ([1]). Similarly
to Kahlermanifolds,
for Kahler foliationsAg
=2~B
holds. Therefore we have the direct sumdecomposition
HrB= ~s+r=r Hs,tB.
We define the operators
L’ : 03A9s,tB - 03A9sB+1, t+
1 andA’ :03A9s,tB - 03A9s,tB- 1’
1by
L’a = ~ A a and A’a =
i(I>’)a.
The basicLaplacian 6B
commutes with L’and A’. Therefore every harmonie basic r-form oc
(r
m +1)
admits aunique decomposition
into a direct sum of the type:where
;.,-2h
are harmonic andeffective
basic(r
-2h)-forms, i.e., A’ )’r- 2h
= 0.In
general,
the basiccohomology H*B(F)
of Fdoes not admit remark- able relations to the de Rhamcohomology H*(M)
of M.However,
for the canonical foliation 57 on a compactg.H.
manifold M there are beautifulrelations between the basic
cohomology
of 57 and the de Rham cohomol- ogy of M([4], [10]).
Let w and B be the Lee form and its dual vector fieldon a
g.H.
manifold M. SinceA(co
Ao)
= w A 0« andLi(B)a
=i (B)~03B1,
every harmonic r-form À has a
unique decomposition
of thefollowing
type:where a,
fi
are harmonic forms andi(B)a
=0, i(B)p =
0. Now we recall thefollowing.
THEOREM 2.3
([4], [10]).
Let M be an n-dimensional compactg.H.
manifold.
For anr-form ). (0
r n -1)
onM, the following
two conditionsare
equivalent:
(i)
À is harmonic, i.e., AÂ= 0;
(ii)
has thedecomposition
À = a + w A(3, where
oc andfi
are basicforms of the canonical foliation
ff andsatisfy AB a = 0, ABfl
=0,
A’a =0, A’fl
= 0(that
is, a and(3
areeffective
harmonicbasic forms of 57).
We denote
by
eh the dimension of the basiccohomology H B h (5). Then, by
thedecomposition (2.5)
of harmonic basicforms,
thefollowing
holds.COROLLARY 2.4
([4], [10]).
On an n-dimensional compactg.H. manifold M,
the Betti numbersbh(M)
aregiven by
I n
particular
thefirst
Betti numberb1 (M)
is odd.3.
Holomorphic
formsIn this section we shall
study holomorphic
forms on compactg.H.
mani-folds. We
keep
the notation in Section 2.Let M be an n-dimensional compact
g.H.
manifold. We denoteby 03A9r(M)
the space
of complex
valued r-forms on M with the scalarproduct , >.
Weconsider the
following
differential operatorsacting
onforms: d, c5, ô, ô, 3, 3, A,
D. Here d = ô+ ô
is the exterior derivative with itsdecomposition
intotwo operators of
bidegrees (1, 0)
and(0, 1). ô, 3,
and3
are definedby
c5 = -
*d*,
3 =-*ô*,
and3
= -*0*, respectively.
Then we have6 = d + ôd
and D
=83
+38
are theLaplacians
of d and0, respectively.
We denote
by e(F)
andi(F)
the exteriorproduct
and the interiorproduct by
the k-formF, respectively.
Inparticular,
we use thefollowing
notation:L =
e«D),
A =i«D),
L’ =e«D’),
A’ =1(O’),
where (D and (D’ are the funda- mental 2-forms of M and of the canonical Kâhler foliationF respectively.
We recall the Lee form w and 0 = - w - J. From
(2.3),
it follows that dO = - (D + w A 0 = - (D’ and ôO = 0. We define the differential form 9 of type(1, 0) by
ç = W +/20131 0.
Then we see thatD(p = 0, 3qJ
= 0 and8qJ = 2013/2013 1
(D’. Infact,
since 0 = dcv =-f(ag
+8qJ
+oip
+ô9),
we haveDg = 8ip
= 0 andD~
+oip
= 0 because of types of forms. Sinceand
we obtain
8qJ = 2013/20131
(D’and3qJ
= 0.By straightforward computation,
we obtain thefollowing:
LEMMA 3.1.
The following
commutationformulas hold for r-forms
on ann-dimensional
g.H. manifold:
We shall
investigate
harmonic forms with respect to U and get thecomplex
version of Theorem 2.3.Namely
we show thefollowing
theorem.THEOREM 3.2. Let M be an n-dimensional compact
g.H. manifold
and ;. adifferential form of
type(p, q)
with p + q n - 1 on M. Then thefollowing
two
conditions for
),. areequivalent:
(1) À satisfies n).
=0,
(2)
À has thedecomposition
À = a +(p 1B f3, where
a andf3
are basicforms of the canonical foliation
F’ andsatisfy D:.Ba = 0, 6Bf3
=0,
A’a =0, A’P
= 0(i.e.
a andf3
areeffective
harmonicbasic forms of F).
Proof.
We first note that any differential form 03BB has aunique decompo-
sition of the
following
type:where
i(g)a = 0, 1(ç)B
= 0. In thedecomposition above,
oc andpare given by p
=)1(ç))w
and a= Â - (0
AB.
From Lemma3.1,
it follows that~e(Ç)
=e(p)~
andDi(cp) = 1(ç)D .
In fact we haveand hence
De(q» = e(q»D. Similarly
we can proveDi(o) = i(g)D Accordingly,
for thedecomposition
03BB, = oc+ 0 n B,
we see that~03BB
= 0 if andonly
if Da = 0 andOP
= 0.Proof of the
implication (2) -(1).
If has thedecomposition
03BB, = oc
+ p 039B03B2 satisfying (2), by
Theorem 2.3 oc andfi
are harmonic forms with respect to A and hencethey satisfy
da =0, d03B2
= 0 and 03B403B1 =0, 03B403B1
= 0.Therefore oc
and 03B2are
also harmonic forms with respect to D.Consequent- ly
we haveQ~,
= 0.Proof of the
implication (1)
-(2).
First wegive
an outline of theproof.
Let oc be a differential form of type
(p, q) (p
+ q n -1)
which satisfies~a = 0 and
1(ç)ce
= 0. Then we shall show that such an « satisfies da =0,
ôa = 0 and hence Aa = 0 and that oc is a basic form of the canonical foliation 5.By
this fact and Theorem2.3,
we see that oc is an effectiveharmonic basic form of F. Thus
combining
this with thepreceding
argument on the
décomposition
= oc+ 0 n B,
we can prove our assertion(1) -(2).
For our purpose, we shall prove the
following key
formula for adifferential form oc of type
(p, q) (p
+ q =r)
which satisfies Qa = 0 and1(ç)03B1
= 0:We note that Da = 0 if and
only
if8a
= 0 and3a
= 0.By
Lemma3.1,
we haveCalculating
the first term of the lastequation,
we obtainCalculating
the third term, we haveTherefore
(3.1)
isproved.
From(3.1),
it follows thatif p + q = r n - 1,
Oli. = 0 and hcnce da = 0. In
particular, if p
+ q = r , n -2, (3.1) implies
that n’a = 0 and
1(Ç)ce
= 0. Next we shall prove that n’a = 0 andi(g)a
= 0hold if p + q = r n - 1. By Lemma 3.1, we have
and hence
On the other
hand,
we haveand hence
Consequently,
if p + q = r n -1,
we have A’« = 0 and1(Ç)ce
= 0. Since1(ç)a
= 0,i(9)a
= 0 and d« =0,
« is a basic form of the canonical foliation ,3F. Sincewe have 03B4a = 0. r-i
As to
holomorphic forms,
thefollowing
holds.THEOREM 3.3. On ann-dimensional compact
g.H. manifold, euery holomor- pl1ic p-.form
asal isjies
cla = 0 and Da = 0. Moreoverif
p n - 1, a is a basicform of the
C’ClilOnIC’Cllfoliation
-5.proof. If I? - ii -
1, we havealready
shown that a satisfies da =0,
Ay - 0 and that a is a basic form of 5. For a
holomorphic
n-form a, (;’Y. = 0 holdstrivially
and hence da = 0. Moreover sincewe have ôa = 0 and hence La = 0. ~ COROLLARY 3.4. On an n-dimensional compact
g.H. manifold,
we haveProof.
The interiorproduct i(V) by
theholomorphic
vector field V is aninjective homomorphism
ofH"’O(M)
intoHn - 1 , ID(M). Conversely
fora c- H"- "’O(M)
qJ A a is aholomorphic
n-form. Infact,
we have8(qJ
Aa)
1 (D’
A oc and since 03A6’ A ce is a basic form of type(n, 1),
we get (D’ A oc = 0 because of types of basic forms. It iseasily
seen that the mapoc
l--+!qJ
n oc ofH5-l,o(M)
intoHô’°(M)
is the inverse ofi(V).
D We denoteby Hâ’9(M)
the Dolbeaultcohomology
group of type(p, q)
and put
hP,q(M) =
dimHp’q(M). Combining
Theorem 2.3 and Theorem3.2,
we get the
following.
THEOREM 3.5. On a compact
g.H. manifold M,
we havebr(M) = Y-p + q = r hp,q(M).
Proof.
We set:Then we have
S’B(ff) = O p+q=r’SB’9( )·
From Theorem 2.3 and Theorem3.2,
it follows thatHr(M; C) SB(F)
Et)SB 1(g;)
for r n - 1 and thatHop""(M) S°q(F)
Qs,q- (F )
for p + q n - 1. Hence for r n -1,
wehave
b,(M) = Lp+q=r hp,q(M). By
Poincaréduality
and Serreduality,
thesame relation holds for r > n + 1.
Using
a result of Frâlicher([3])
whichstates that
we can prove
bn (M) - p + 9 - n h’9(M).
DRemark
3.6.,
Theorem 3.3 and Theorem 3.5 show that the same resultsas in the case of compact Kâhler manifolds hold on compact
g.H.
manifolds. But the relation
hP,q(M) = hq,p(M)
is not true on a compactg.H.
manifold. For
example
we have h°’’’ =hP’o
+hP- 1,0
for p n - 1. Inparticular,
we have h1,o =!(b1 - 1)
and h°° =2(b
1 +1).
4.
Holomorphic
vector fieldsIn this
section,
we shallinvestigate holomorphic
vector fields on a compactg.H.
manifold.Let F be the canonical foliation of a
g.H.
manifold M with tangent bundle L and normal bundleQ
of F and n denote theprojection
TM -Q.
Usually
weidentify Q
with theorthogonal complement
L.l of L.By
Lemma2.1(2), V
= B -1 A
is aholomorphic
vector field with no zeropoints
and hence L+ is a
holomorphic
subbundle of TM +. Thus thequotient
bundle
Q + = TM +/L+
is aholomorphic
vector bundle and n :TM’ --+ Q’
is a bundle
homomorphism
betweenholomorphic
vector bundles. If X is aholomorphic
vector field on M, thenn(X)
is aholomorphic
section ofQ +.
Now,
we shall discussholomorphic
sections ofQ +.
Let us recall theunique
metric and torsion-free connection V’ induced inQ
and also inQ + .
Then V’ is a connection
of
type(1, 0)
on theholomorphic
vector bundleQ +,
i.e.,
a connection which maps localholomorphic
sections inQ +
ontoQ +-valued
forms of type(1, 0).
Inparticular,
V’ is a Hermitian connection of theholomorphic
Hermitian vector bundle(Q +, gQ), where gQ
is aninduced
holonomy
invariant metric onQ.
Thus for a section X ofQ +, X
is
holomorphic
if andonly
ifVyX
= 0 for any Y E rTM +.Let ç
be thecorresponding complex
differential 1-form toX E hQ +
definedby j(Y) = gQ(X, Y)
for Y ErQc. Then ç
is of type(0, 1)
and we see that X is aholomorphic
sectionof Q +
if andonly if ’V =
0 for any Y E rT M + : We denotesimply by ç
the 1-formn*ç
of type(0, 1)
on M.For later
convenience,
we present the relation between the connectionsV’, V,
andV,
where Vand V
denote the Riemannian connection and theconnection defined
by (2.1) respectively:
where X, Y E
r(L1)c
and V =B - l
A. In theabove,
weidentify Q
with Ll.
PROPOSITION 4.1.
If ç is
the1-form of
type(0, 1) corresponding to a holomorphic
section X ErQ +,
we haveôj
= 0.Proof. Using (4.1),
we haveand
for
Y, ZEr(L1.)+.
~THEOREM 4.2.
Any holomorphic
section Xof Q+
on a compactg.H.
manifold
M is aholonomy
invariant section with respect to 57.Proof Let ç
be the 1-form of type(0, 1) corresponding
to X. Then it is sufficient to provethat ç
is a basic form of 57.By Proposition 4.1,
we canwrite ç as ç = Ço
+ôg
whereÇo
satisfiesDço
= 0 andf
denotes acomplex-valued
function on M.Since Di(ç)j
=i(qJ)Dç 0
=0, i(qJ)ç 0
=ço(V)
is a constant function on M. Thus we havewhere
vol(M)
denotes the volume of M. Sincewe obtain
i(qJ)ç 0
= 0. From Theorem3.2,
it follows thatÇo is
a basic formof F. Moreover we have
Vf
=1(ç)j - i(qJ)ç 0 =
0. This means that thefunction
f
isholomorphic
on each leaf of 57.By
Lemma2.1,
the universalcovering
of each leaf isbiholomorphic
to C. Sincef
isbounded, f
is aconstant function on each leaf and then
f
is a basic function of F’. Thus it has beenproved that ç
is a basic form of 57. D From thepreceding theorem,
it follows that theI-form ç corresponding
to a
holomorphic section
Xof Q +
determines a basic Dolbeault cohomol- ogy class[ç]
EH’,’(F).
For aholomorphic
section X ofQ +,
Vaisman in[10]
constructed aô-closed
1-formK(X)
of type(0, 1),
which is related to ourI-form ç by -2[K(X)] = [ç]
inHP@’(M).
Moreover he answered thequestion
whether there exists aholomorphic
vector fieldX
of M such thatneX-)
= X in terms of its Dolbeaultcohomology
class[x(X)] (Theorem
4.5in
[10]).
Now we shall answer the samequestion
as above in terms of itsbasic Dolbeault
cohomology
class[ç].
THEOREM 4.3. Let X be a
holomorphic
sectionof Q +
with thecorrespond- ing I-form ç
on a compactg.H. manifold
M. Then there exists aholomorphic
vector field X on
M such thatn(X)
= Xif and only if [c;]
= 0 inHo,’(J’).
Proof.
For agiven holomorphic
sectionX E rQ +,
any vector fieldX
of type(1, 0)
on M such thatn(X)
= X is writtenas X
= X +f V,
wheref
denotes some differentiable function on M. Here we identified
Q +
with(L1.) + . Noticing
that theconnection V
is of type(1, 0),
we see thatX
isholomorphic
if andonly
ifVyX
= 0 for any Y Er(L1) + and
= 0.Using (4.2),
we calculatefor
YEr(L1.)+
andIf X is a holomorphic
vectorfield, by
the secondequation
in the above, weobtain
ô f ( V )
= 0 andby
the argument in theproof
of Theorem 4.2, we see thatf
is a basic function of 5. From the firstequation,
it follows thatç = -28Bf
and hence[ç]
= 0 inH’,’(F).
The converse iseasily
seen. D COROLLARY 4.4. Let M be a compactg.H. manifold
withb1(M) =
1. Thenfor
anyholomorphic
section X EFQ +,
there exists aholomorphic
vectorfield X
such thatn(X)
= X.Proof.
Ifb1(M) =
1, a result obtained in Section 3implies
thatHo,’(57)
={O}.
~We denote
by
2( thecomplex
Liealgebra consisting
of allholomorphic
vector fields on M. Then on a compact
g.H.
manifoldM,
we haveMoreover the
following
holds:COROLLARY 4.5.
{cVlcEC} is
contained in the centerof
21.Proof.
We note that[ V, X ] E I’(L1) +
for anyX E r(L1) + .
From theargument in the
proof
of Theorem4.3,
it follows that for anyX E 21 X
is writtenas X
= X +f V,
where X is aholomorphic
sectionof (L1)+ ^, Q+
and
f
is a basic function of 5.By
Theorem4.2,
X is aholonomy
invariantsection of F’. Therefore we obtain
[ V, X]
= 0. DNow we shall show an
analogous
result to a theorem of Matsushima and Lichnerowicz. We denoteby Sl
the real Liesubalgebra
of 21consisting
ofholomorphic
vector fields whose associated real vector fields areKilling
vector fields. Then we have the
following.
THEOREM 4.6. Let M be a compact
g.H. manifold
with constant scalarcurvature. Then we have
where V = B -
V/---l
A is a vectorfield given
in Lemma2.1(2).
Proof.
In theproof
of thistheorem,
the canonical foliation alsoplays
animportant
role.First,
we review basicproperties
oftransversally holomorphic
sections of Kàhler foliations(cf. [5]).
Let F be a Kâhler foliation on a manifold M.We denote
by V(F)
andrQL
the Liealgebra
of infinitesimal auto-morphisms
of F and that ofholonomy
invariant sections of the normal bundleQ, respectively.
Then we have an exact sequence of Liealgebras:
which is associated with
(2.4) (cf. [6] Chap. 9).
For Kâhlerfoliations,
thespace
1-(Q ’)’
ofholonomy
invariant sections of type(1, 0)
is a Liesubalgebra
ofr(QC)L.
A sections E I-’(Q +)L
is said to betransversally
holomorphic
if its associated real section u = s + s satisfiesLYuJQ
=0,
where
n(Yu)
= u. We denoteby
9T thecomplex
Liesubalgebra
ofh(Q +)L
consisting of transversally holomorphic
sections. GivenSE r(Q + )L,
we seethat sE21’ if and
only
ifVyS
= 0 for anyYEr(L1.)+.
A sectionSErQL
issaid to be
transversally Killing
ifLYsgQ
= 0 holds. Then s EFQL
is trans-versally Killing
if andonly
if it satisfiesgQ(V’ x s, 7r(Y»
+gQ(n (X), Vys)
= 0for any X, Y E rLl. We denote
by R’
the real Liesubalgebra
ofhQL consisting
oftransversally Killing
sections. From now on, we assume that M is compact and orientable and that 57 is harmonic. Thensimilarly
tothe case of compact Kâhler
manifolds,
we see that if u is atransversally Killing section,
its associated section s =2(u - J=1 J QU)
oftype (1, 0)
istransversally holomorphic (cf.
Theorem B in[5]).
Inparticular,
R’is identified with a real Lie
subalgebra
of 21’.Moreover,
Nishikawa andTondeur
generalized
a theorem of Lichnerowicz to the foliation context.To state this
result,
we recallcomplex
Liesubalgebras
0’ and (--Ç’of 9r :
0’, by definition,
is the ideal of 21’consisting
oftransversally holomorphic
sections whosecorresponding
basic(0, 1)-forms
vanish inH’,1(F);
OE’ is the Liesubalgebra
of 9Tconsisting
oftransversally holomorphic
sections which areparallel
withrespect
to V’. Then thefollowing
holds.THEOREM 4.7
(Theorem
D in[5]).
Let 5’ be a harmonic Kâhlerfoliation
on acompact
orientablemanifold
M with constant transversal scalar curvature. Then we haveNow we return to the
proof
of Theorem 4.6. Let F be the canonical foliation of a compactg.H.
manifold M. Let X be aholomorphic
sectionof the
holomorphic
vector bundleQ +.
From Theorem4.2,
it follows thatX is a
holonomy
invariant section. Moreover sinceVyX
= 0 for anyYEFTM’, X
istransversally holomorphic. Conversely
if X is a trans-versally holomorphic
section ofQ+,
we haveVpX
= 0(V
= B -1 A)
and
VpX
= 0 for any Y Er(L1.) + . Consequently
X is aholomorphic
sectionof
Q + .
Therefore 9T coincides with the space ofholomorphic
sectionsof Q + .
The
projection
n is a Liealgebra homomorphism
of thecomplex
Liealgebra
2t of allholomorphic
vector fields on M into 21’. Let X be aholomorphic
vector field which satisfiesn(X) =
0. Then X is written asX =
f V,
wheref
is aholomorphic
function on M. Since M is compact,f
is constant. Therefore we have ker n =
{c Vie E CI.
From Theorem4.3,
itfollows that
n(2I) =
0’.Next we shall prove the
following.
L E M M A 4.8. For
X E 21, X belongs to R if and only if n(X) belongs
to R’.Proof.
We denoteby W
the real vector field associated to X.W
isdecomposed
intoW
= W +fiB
+f2A,
where WErLJ.. Let us denoteby
â and oc the dual 1-forms
corresponding
toW and W, respectively.
Then wehave à = a +
ficv
+f20.
From the argument in theproof
of Theorem4.3,
it followsthat f1 and f2
are basic functions of F and that a =- df1
+d f2 J
holds.W
is aKilling
vector field if andonly
if thefollowing equations
hold:for
any Y,
Z E r L 1..Since f1 and f2
arebasic,
theequation (1) always
holds.The
equations (2)
and(3)
hold if andonly
iffl
is constant on M. Infact,
we have
The
equation (4)
isequivalent
to(V’yoe)(Z)
+(Vz(x)(Y)
= 0for Y,
Z E rL1..I n fact we have
Therefore if
X E R,
the real vector field W associated ton(X)
is trans-versally Killing. Conversely
suppose that W istransversally Killing.
Then(Vy(x)(Z) + (Va)( Y) = 0
forany 1": Z E r L 1.
and hencebB(X = o.
SincebB(df2 oJ)=bB(dBf2 oJ)=O,
we have~B.f1 =bBdBfI = -bBa+bB(df2 O J) = 0
and
hence , f’1
is a constant function. ThereforeW
is aKilling
vectorfield. D
We continue the
proof
of Theorem 4.6. We have thefollowing
relationbetween the scalar curvature T and the transversal scalar curvature T’
of !F: T = --!(n - 1)
+ T’.Applying
Theorem4.7,
wecomplete
theproof
ofTheorem 4.6.