A NNALES DE LA FACULTÉ DES SCIENCES DE T OULOUSE
S AMUEL I. G OLDBERG
I ZU V AISMAN
On compact locally conformal Kaehler manifolds with non-negative sectional curvature
Annales de la faculté des sciences de Toulouse 5
esérie, tome 2, n
o2 (1980), p. 117-123
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ON COMPACT LOCALLY CONFORMAL KAEHLER
MANIFOLDS WITH NON-NEGATIVE SECTIONAL CURVATURE
Samuel I. Goldberg(1)(*) and Izu Vaisman (2)
Annales Faculté des Sciences Toulouse
Vol II, 1980, P. 117 à 123
(1 ) University
ofIllinois, Urbana,
Illinois - Etats Unis.(2) University
ofHaifa,
Haifa - Israe’I.Resume : Une variété
compacte, localement,
mais pasglobalement,
kählérienneM,
à forme deLee w
jamais
nulle et à courbure de Riccipositivement
semi-définie et s’annulant dans la direc- tion de B =# w seulement,
a la forme de Leeparallèle. Si,
deplus,
M estrégu lière
et a la courbu-re
non-négative
et la courbure sectionnelle sur w = 0positive,
alors elle ales nombres de Bettib~ (M) = 1,b~(M)
= 0.Si,
encore deplus,
M estquasi-Einstein
et si elle al’espace
des feuillesM/B simplement
connexe, M est une variété deHopf.
Summary :
Acompact locally,
but notglobally,
conformal Kaehler manifold M with nowherevanishing
Lee form w, and with apositive
semi-definite Ricci tensor which vanishes in the direction of B =#
wonly,
has aparallel
Lee form.If,
moreover M isregular,
and has non-negative
curvature andpositive
sectional curvatures on w =0,
it has the Betti numbersb~ (M) = 1,b~(M)
= 0.And,
if we also add thehypotheses
that M isquasi-Einstein
and has asimply
connected leaf space
M/B,
then M is aHopf
manifold.1- INTRODUCTION
A
locally
conformal Kaehlermanifold,
henceforth called an 1. c. K.manifold,
is an Hermitian manifold(M, J, g)
ofcomplex
dimension m >2,
whereJ2=-I
andg(JX,JY) =g(X,Y),
for which an open
covering ~ U« ~ exists,
and for each a a differentiable functiono : U -~ IR,
(*) This paper was written while the author was a Lady Davis Visiting Professor at the Technion- Israel Institute of Technology, Haifa, during the Spring of 1979.
118
such that e
a°~(g I U )
is a Kaehler metric onUQ,
called alocally
conformal Kaehler metric. It is then easy to see[7]
thatw I U Q
= dQ «
defines aglobal
closed1-form,
and that M has the cha- racteristicproperty
d Q = w A S~ where =g(X, J Y)
is the fundamental form of M. If we can takeU«
=M,
the manifold isglobally
conformal Kaehler(g.
c.K.).
The form w is called theLee form of M. It is exact if and
only
if M is g. c. K. An 1. c. K. manifold is said to beregular
ifthe
trajectories
of the Lee vector fieldB,
definedby
w =g(B; ), provide
aregular
foliation Bon
M , with
a Hausdorffquotient
manifoldM/B.
Denoting by K(s)
the sectional curvature of the 2-section s, we say that an 1. c. K.manifold has
positive
horizontal sectional curvature ifK(s)
> 0 whenever s isorthogonal
to B. An1. c. K. manifold is called
quasi-Einstein
if its Ricci curvatureQ
isgiven by Q
= ag + b w ® w forsome functions a and b on M.
Pertinent
examples
areprovided by
theHopf
manifolds with the metric derived from thediffeomorphism
with x51 [7,8] .
Let us recall that these are defined asquotient
manifolds H =
(Cm - {0}) / 0394k ~ S2m-l
xS 1 where 0394k
is the transformation group gene- ratedby z~
-~kz’ (i=1,...,m), I k I ~ 0,1
and(z’)
E~m - ~ 0 ~ .
For m >1,
the second Betti num- berb2(H)
=0,
so H is not Kaehlerian. Its natural 1. c. K. metric is[2,p.167 ;7,8]
with the fundamental form
satisfying
= 03C9 03A9 for the Lee formwhich is
closed,
not exact and it has no zeroes.Using
results of[8],
it follows that H is acompact
1. c. K. manifold withnon-negative
curvature and horizontalpositive
sectional curvature, whose metric isquasi-Einstein
and whose Ricci curvature vanishes in the direction of Bonly.
The purpose of this paper is to
give
thefollowing
differentialgeometric
characteri- zation of theHopf
manifolds.THEOREM.
(i)
Let M be a compact connectedregular
1. c. K. manifold which is not g. c. K.and has
non-negative
curvature and horizontalpositive
sectional curvature. 1 f its Ricci curvature vanishes in the direction of Bonly,
then b1 ( M )
=1 andb 2 ( M )
=0 ;
(ii) lf,
moreover, M isquasi-Einstein
and the leaf space MI
B issimply connected,
Mis a
Hopf
manifold.2 - THE LEE FORM
That
Q
vanishes in the direction of Bonly
isrequired
in order to ensure that the Leeform is
paral lel.
Indeed,
we have thefollowing.
PROPOSITION 2.1. Let M be a
compact
1. c. K. manifold with Lee form W ~ 0everywhere,
and which is not g. c. K.
Then,
if its Ricci tensor ispositive semi-definite,
and vanishes in the direc- tion of Bonly,
W isparallel.
Proof. Let
be the
Hodge decomposition
of ~, where h is its harmonicpart.
SinceQ
ispositive semi-definite,
h is covariant constant
(see [2,p.87] ),
and so from(2.1)
where
7.
denotes the covariant derivativeoperator
with respect to the Levi Civita connection in the direction of the natural basis vectorThe
integrability
condition of(2.2)
iswhere the are the
components
of the curvature tensor withrespect
to the natural basis.Hence, by
contractionP~( ~j - = 0,
that is Q(B-F,X)
= 0 for every X
where df=g(F, .).
In
particular, Q(B-F,B-F)
=0,
so sinceQ
vanishes in the direction of Bonly,
we must haveAssume 03BB ~ 1.
Then, (2.3) yields
for some function p . Since w is
closed, d Jl
A df =0,
and because W does not vanish any~where, df ~ 0 everywhere.
We therefore haved p
= p df.Again,
sincedf =~=
0everywhere,
wesee
that p depends only
onf,
soby (2.4),
w is exact. Since M is not g. c.K.,
this isimpossible.
Hence, X
= 1 and f = const.Thus,
from(2.1),
w isharmonic,
and thereforecovariantly
constant.Remark. The condition w =f=. 0 at every
point
says that the Euler-Poincaré characteristic of M vanishes.Proposition
2.1 hasimportant
consequencesincluding
the fact thatbl (M)
is odd[4].
.Moreover,
we can provePROPOSITION 2.2. Let M be a
compact
connected non-Kaehler 1. c. K. manifold withparallel
Lee form.
Then, (i)
if a is acovariantly
constantp-form
onM,
a = kw(k
=const.)
for p=1,
,and a = 0 for
2 ~ p
2m -2, d i m~
M = m(ii)
I f the Ricci curvature ispositive semi-definite,
then
b1(M)=1.
.Proof.
(ii)
is astraightforward
consequence of(i),
and of the well-known fact(already used)
that aharmonic 1-form on a compact Riemannian manifold with
positive
semi-definite Ricci curvature is covariant constant.To
get (i),
we shall use a resu lt of Kashivada and Sato[4]
andadapt
acomputation
of Blair and one the authors[
1]. Namely,
if we set A = -J B,
wehave, by
theproof
in[4]
and inanalogy
with a known result for Sasakian manifolds[6],
thati(A)a
= 0 for every harmonicp-form
a with p m. ln
particular,
this is true for thecovariantly
constant forms a.(i(X)
denotes the in- teriorproduct by X).
.Furthermore,
if we w oJ,
thefollowing
formula isimplicit
in[4]
and[8]
Since for the a we consider
i( = 0, (2.5) yields
or
equivalently
Here, I w I =
const. =1= 0 since M is not Kaehlerian. For p= 1,
thisyields
a = k w(k
=const.).
For 2
p m - 1,
if weput
X = X’ + XB with w(X’)
=0,
weget a(X’,Y1,...,Yp-1 )
=0,
andif
Y., = Vl + Il B
withw (Y~ ) = 0,
we obtaina(B,Y1,...,Y p -1 ) = a(B,Y~,Y2,...,Yp-1 ). Thus, Aa(B,Y1,...,Y p -1 ) - Aa(B,Y~,...,Yp_1 ) _ - Aa(Y~,B,...,Yp-1 ) =
0. SinceV a = 0
implies V (*a)
=0,
where * is theHodge
staroperator, a
= 0 for m + 1p
2m - 2also.
Finally,
for p = m, we consider the form w A a which iscovariantly
constant and ofdegree
m + 1. Therefore it must be zero. It follows
that ! I
w12
c~= w Ai(B)a=
0 sincei(B)a
is cova-riantly
constant and ofdegree
m -1.This
completes
theproof
ofProposition
2.2.3 PROOF OF THEOREM
We now prove the theorem formulated in Section 1. We
begin by noting that,
underthe
hypotheses,
and in view ofProposition 2.1,
the Lee form isparallel.
Thegeometric
structureof such manifolds has been studied
by
one of the authors in[8] ,
where thefollowing
basic factswere obtained.
First,
theequation
m = 0 defines a codimension one foliation ofM,
whose leaves L aretotally geodesic
submanifolds and inherit from M ageneralized
Sasakian structure(see below). Second,
because of theregularity
of the foliation B(see
Section1),
thisgives
rise to anS1-principal
fibration p : M -~S,
S =M/B,
which is flat(with
connectioncj )
and is such thatp I L :
L -~ S is acovering
map for any leaf L defined above. This leads to ageneralized
Sasakianstructure on S.
By
ageneralized
Sasakian structure we understand here a normal contact metric structure[6]
whose contact form 17 and fundamental form 4) are relatedby d n - I w
I~ ,
where I
w I = const. This is a Sasakian structureif I
wI =1.
Now,
since L isorthogonal
to B and it istotally geodesic,
ithas,
in our case,positive
sectional curvature.
Thus,
the same is true forS,
andbl (S)
=b2(S)
= 0 followby
a known theo-rem
[5,6]
ifI w I =1. Moreover,
in the samecase, S
is asphere
if it is asimply
connected Einsteinmanifold
[5,6] .
The same results are trueif I w | ~
1 since this case can be reducedby
a homo-thetic
change
to theprevious
one, whilepreserving
thehypotheses.
Furthermore,
since the fibration p isflat,
it hasvanishing
Eulerclass,
and hence avanishing Gysin
map. It then followseasily
form theGysin
sequence thatfrom which
(i)
follows.To prove
(ii),
it is sufficient to note that since L istotally geodesic
and M isquasi- Einstein,
S is Einstein.Therefore, S
is asphere
and M can be identified with theproduct
of thissphere by S1 (see
also[8] ).
In connection with the last
part
of theTheorem,
we also provePROPOSITION 3.1. A
compact
connected non-Kaehler 1. c. K. manifold withparallel
Lee formis
quasi-Einstein
if andonly if,
the Ricci curvatureQ
of thelocally
conformal Kaehler metricsg
vanish. In this case, the Ricci tensor
Q
isgiven by
and it is
positive
semi-definite.Proof. Since g and
g are conformally
related and K7 cJ =0,
a well-known formula[2, p.115] gives
This shows that the stated condition is sufficient.
Conversely, (3.3) gives
Since
g is
a Kaehlermetric, ~ (X,Y)
=Q(X,JY)
isskew-symmetric,
and thisimplies
b=-(m-1 )/2.
Since ~
isclosed,
d v A S~ + v d St = o. But d S~ = w A S~and 12
isnon-degenerate,
soIf 03BD ~ 0
everywhere, 03C9
would be exact and M would thereforebeg.
c. K. This isimpossible
since
by [4] , bl (M)
is odd. On the otherhand,
if u vanishes at apoint x~,
it isidentically
zero.Indeed,
cj =d/
aboutx0,
so from(3.4),
v =c/
T for some constant c. Since v(xo)
=0,
cis zero.
Thus,
v(x)
= 0 for all x E M as one seesby propagating
the local resultalong
a chain ofconsecutive
intersecting neighborhoods joining x 0
to x.But,
u = 0 means a =(m-1 ) I w 1 2 /
2.The Ricci tensor is therefore
given by (3.2).
123
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