J. Korean Math. Soc. 32 (1995), No. 3, pp. 553-562
CRITICAL RIEMANNIAN METRICS ON COSYMPLECTIC MANIFOLDS
BYUNG HAK KIM
1. Introd uction
In a Recent paper [3], D. Chinea, M. Delon and J. C. Marrero proved that a cosymplectic manifold is formal and constructed an example of compact cosymplectic manifold which is not a global product of a Kaehler manifold with the circle. In this paper we study the compact cosymplectic manifolds with critical Riemannian metrics.
Let M be an m-dimensional compact orientable Riemannian man- ifold and J..Io( M) be the set of Coo Riemannian metric G on M satis- fying fM dVa = 1, where dVa is the volume element of M measured by G. For an element G in J..Io(M), we assume that f(k) is a scalar field on M determined by G as the contraction of a tensor product of the curvature tensor. Then HM[G] = fM f(k)dVa defines a mapping H M : J..Io( M) -+ R. In this case, a critical point of H M is called a critical Riemannian metric with respect to the field f( k) and denoted by G H.
The following four kinds of critical Riemannian metrics have been studied by M. Berger [1] and Y. Muto [7] :
AM[G] = fM K dVa,
CM[G] = fM S2 dVa,
BM[G] = fM K 2 dVa,
DM[G] = fM R 2 dVa,
Received July 5, 1994.
1991 AMS Subject Classification: 53C20.
Key words: Critical Riemannian metrics, fibred Riemannian space, cosymplectic manifold.
This research was partially supported by TGRC-KOSEF and the Basic Science
Research Institute Programs, Ministry of Education, 1994.
where R, S and K are the Riemannian curvature tensor, Ricci curva- ture tensor and scalar curvature respectively. The equations of the critical Riemannian metrics are written as follows:
(1.1) Aji =CAGji,
Cji =CCGji,
Bji = CBGji, Dji = CDGji,
where CA, CB, Cc, CD are undetermined constants and Aji,Bji,Cji and D ji are given by
(1.2) (1.3)
(1.4)
(1.5)
Aji = -Sji + '2K Gji, 1
Bji = 2\ljViK - 2(b.K)Gji - 2K Sji + ~K2 Gji,
" 1
Cji =\lj\liK - \l"\l Sji - i(b.K)Gji - 2RjkhiS kh + %SkhSkhGji,
Dji =2VjViK - 4V"V k Sji + 4SjkSi k
4R S kh 2R R HI 1 R RkhlmG
- jkhi - j/ohl i +"2 khlm ji,
where V is the Riemannian connection and b.K is the Laplacian of K with respect to G on M.
2. Cosymplectic Bochner curvature t~nsor
Let M be an m-dimensional cosymplectic manifold with structure
(q,,~,.'1, G), that is, a manifold M which admits a I-form "l, a vector fields ~, a metric tensor G satisfying
"l(e) = 1, q,2 X = -X + "l(X)e, q,e = 0,
G(e,X) = "l(X), G( q,X, q,Y) = G(X, Y) - "l(X)"l(Y)
Critical Riemannian metrics on cosymplectic manifolds 555
and ~(X, Y) = G(cPX, Y) and TJ are both closed for arbitrary vector fields X and Y on .M. The relations
'VeK = 0 and R(X, Y)~ = 0 are easily verified.
The cosymplectic Bochner curvature B is defined by B(X,Y,Z,U)
=R(X, Y, Z, U) + {G(X, U) - TJ(X)TJ(U)}L(Y, Z)
- {G(Y, U) -1J(Y)1J(U)}L(X, Z) + {G(Y, Z) - TJ(Y)1J(Z)}L(X, U) - {G(X, Z) - 1J(X)1J( Z)}L(Y, U) + q>(X, U)M(Y, Z)
- ~(Y, U)M(X, Z) + q>(Y, Z)M(X, U) - q>(X, Z)M(Y, U) - 2{q>(Z, U)M(X, Y) + q>(X, Y)M(Z, U)},
where we have put
L(X,Y) = (1 )[S(X,Y)+o:{G(X,Y)-TJ(X)7J(Y))], 2 m+2
M(X, Y) = -L(X, cPY) and
o:=-~-~
K 4(m + 1)
We assume that the cosymplectic Bochner curvature B vanishes iden- tically on M, then we get
(2.1)
R(X,Y,Z,U)
=~3 [S(Y, Z){G(X, U) - 1J(X)1J(U)}
m+
-SeX, Z){G(Y, U) - TJ(Y)1J(U)}
+S(X, U){G(Y, Z) - 1J(Y)7J(Z)} - S(Y, UH G(X, Z) - TJ(X)1J(Z)}]
- (m + 1)(m K + 3) [{G(Y, Z) - TJ(Y)TJ(Z)}{G(X, U) - TJ(X)7J(U)}
- {G(X,Z) - TJ(X)77(Z)}{G(Y,U) - TJ(Y)1J(U)}]
- q>(X, U)M(Y, Z) + q>(Y, U)M(X, Z) - q>(Y, Z)M(X, U)
+ q>(X, Z)M(Y, U) + 2{ q>(Z, U)M(X, Y) + q>(X, Y)M(Z, U)}.
LEMMA 2.1. litbe cosymplectic Bocbner curvature B oftbe cosym- plectic manifold M vanisbes identica.11y and M is Einstein, tben M is locally Euclidean.
Proof. From (2.1), we easily get
SeX, Y) = {-!..G(X, Y) - (4 ) T/(X)q(Y)}K.
m mm+3
This equation implies K = 0 and that S = o. Then we get R = 0 by use of (2.1).
If the scalar curvature vanishes on M, then, from (2.1), we have (2.2)
R(X,Y,Z,U)
=~3 [S(Y; Z){G(X, U) - q(X)T/(Un
m+
-sex, Z){G(Y, U) - T/(Y)q(U)}
+S(X, U){G(Y, Z) - q(Y)q( Z)} - S(Y, U){ G( X, Z) - q( X)7](Z)} 1
- «p(X, U)M(Y, Z) + CP(Y, U)M(X, Z) - «p(Y, Z)M(X, U) + cP(X,Z)M(Y,U) + 2{cP(Z,U)M(X,Y) + cP(X,Y)M(Z,U)}.
Thus we can state
LEMMA 2.2. li tbe cosymplectic Bocbner curvature Band tbe scalar curvature vanisb on tbe cosymplectic manifold M, tben tbe curvature tensor on M is of tbe form (2.2).
3. Cosympleetic manifold with critical Riemannian metrics Let M be an m-dimensional cosymplectic manifold. If the Riemann- ian metric G is a critical Riemannian metric GB, Gc or G D, then, by use of (1.1)-(1.5), the undetermined constants CB, Cc and CD given by (1.1) are determined as follows :
1 2
(3.1) CB ="2K - 2~K,
1 .. 1
(3.2)· Cc =-S·-B 2 JZ Jz - -~K 2 '
1 kOOh
(3.3) CD =-RkjihR JZ •
2
Critical Riemannian metrics on cosymplectic manifolds 557
From (1.1), (1.3) and (3.1), we get
VxVyI( = K S(X,Y).
Then
fM K 2 dVGB = fM ~K dVGB'
Thus, applying the Green's Theorem, we have
PROPOSITION 3.1. In a compact cosymplectic manifold M, G is a critical Riemannian metric GB on M if and only if tbe scalar curvature vanishes.
By use of (1.4) and (3.2), we have
PROPOSITION 3.2. In a cosymplectic manifold M, G is a critical Riemannian metric Gc on M ifand only iftbe Ricci curvature vanishes.
If the Riemannian metric G on M is the critical Riemannian metric G D, then we obtain
by use of (1.5) and (3.3). Thus we have
PROPOSITION 3.3. In a compact cosymplectic manifold M, G is a critical Riemannian metric G D on M if and only if M is locally Eu- clidean.
From (2.1), we easily see that the cosymplectic manifold with van- ishing cosymplectic Bochner curvature is locally Euclidean if the Ricci curvature vanishes. Moreover, it is well known that if G is a critical Riemannian metric GA, then G is an Einstein metric. From these facts and Lemma 2.1, Propositions 3.2 and 3.3, we have
PROPOSITION 3.4. The compact cosymplectic manifold with van-
islllng cosymplectic Bocbner curvature is locally Euclidean if and only
ifC is a critical Riemannian metrics CA or Gc or CD.
4. Critical Riemannian metrics in the fibred Riemannian space
Let {M,B,G,7r} be a fibred Riemannian space, that is, {M,G}
is an m-dimensional total space with projectable metric G,B an n- dimensional base space and 7r : M -+ B the projection with maximal rank n. The fibre passing through a point q E M becomes an p(= m - n )-dimensional submanifold of M, which is denoted by F q or generally F. Throughout this section, the ranges of the indices are as follows :
h,i,j,k,l = 1,2,··· ,m,
a,b,c,d,e = 1,2,··· ,n,
a,f3,~,6,€=n+1,··· ,n+p=m, unless stated otherwise.
Let {EO!, CP} be dual to the frame {Eb, COl} of M and denoting R kii h components of the curvature in M, we have the structure equation as follows [2, 4, 5, 8] :
(4.3) RhP = RhP + h6/h..,
O!e -h r /h 6 0!e,
where R de6a and R hP are the components of the curvature in B and F respectively, h = (hp:) and L = (LcbO!) are the components of the second fundamental tenSor and normal connection of each fibre F respectively, arid we have put
,
Rdcba =G(R(Ed' Ec)Eb, Ea),
R d..,';, =G( R( E d ; C.., )E b , COl), R6 ..,p =G(R(C6, C..,)CP, COl),
*V dhl\ =8dhlb - rdbhle + QdEO!hl b - QdphEO!b'
**V..,Lcb =8dhcbO! - rdcLebO! - r:bLceO! + QdEO!Lcb
E,Qcl =PepO! - hPO!e,
Critical Riemannian metrics on cosymplectic manifolds 559
Pel' are local function related to Le", GP = P d ! E d and P3e is the
Christoffel symbol induced by the metric in B.
Denoting by Sji components of the Ricci tensor in M, then we have [2,4,5, 8]
(4.4)
Seb = S(Ee,Eb) =Seb - 2Le/L b e
E -