C OMPOSITIO M ATHEMATICA
Y OSHIHIRO O HNITA
On stability of minimal submanifolds in compact symmetric spaces
Compositio Mathematica, tome 64, n
o2 (1987), p. 157-189
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157
On stability of minimal submanifolds in compact
symmetric spaces
YOSHIHIRO OHNITA
Department of Mathematics, Tokyo Metropolitan University, Fukasawa, Setagaya, Tokyo, 158, Japan (current address until 1 September 1988: Max-Plank-Institüt für Mathematik, Gottfried Claren-Strasse 26, D-5300 Bonn 3, FRG)
Received 22 January 1987; accepted 8 April 1987
Dedicated to Professor Ichiro Satake on his 60th birthday
Compositio (1987)
© Martinus Nijhoff Publishers, Dordrecht - Printed in the Netherlands
Introduction
A minimal
subvariety
M of a Riemannian manifold N is called stable if the second variation for the volume of M isnonnegative
for every variation of M in N. Stable minimal subvarieties incompact
rank onesymmetric
spaceshave been classified
(cf. [S], [L-S], [01], [H-W]).
It is aninteresting
andimportant problem
to find all stable minimal subvarieties in eachsymmetric
space. In this paper we discuss the
stability
of certain minimal subvarieties incompact symmetric
spaces. First we reformulate thealgorithm
of deter-mining
the indices and nullities ofcompact totally geodesic
submanifolds incompact symmetric
spaces(cf. [C-L-N]). Using
this method we determine the indices and nullities of allcompact totally geodesic
submanifolds incompact
rank onesymmetric
spaces andHelgason spheres (cf. [H1])
in allcompact
irreduciblesymmetric
spaces. Moreover we prove a nonexistence theorem for stable rectifiable currents of certaindegree
on somesimply
connected
compact symmetric
spacesby
the method of Lawson and Simons[L-S].
1. Jacobi
operator
of minimal submanifoldsLet M be an m-dimensional
compact
minimal submanifold(without
bound-ary)
immersed in a Riemannian manifold(N, h)
and denote the immersionby
cp: M ~ N. If the second derivative of the volume Vol(M, cp*h)
at t = 0is
nonnegative
for every smoothvariation {~t]
of cp with cpo = cp, then wesay that cp is stable and M is a stable minimal submanifold of N. We denote
158
by g, A, B, Vi.
andR’
the Riemannian metric on M induced from hthrough
9, the
shape operator,
the second fundamentalform,
the normal connectionof cp and the curvature tensor of
(N, h), respectively.
For any vector field V Er(cp-1 T(N))
we choose a smoothvariation {~t} of ~ with go
= 9 and the variational vector field(~/~t)~t(x)|t=0 = Vx (x
EM).
Then the classicalsecond variational formula is
given
as follows(cf. [S]);
where dv denotes the Riemannian measure
of (M, g)
and VN thecomponent
of V normal to M.Hère 3
is defined aswhere
41 - Emi=1 ~~2el,el
andA~, R~
are smooth sections of End(N (M))
defined
by ~A~(u), 03C5~ = Trg(AuA03C5), ~R~(u), 03C5~ = Em ~RN(ei, u)ei, v i
for u, v E
Nx(M). {ei}
denotes an orthonormal basis ofT, (M). 3
is a self-adjoint strongly elliptic
linear differentialoperator
of order 2acting
on thespace
F(N(M»
of all smooth sections of the normal bundleN(M),
calledthe Jacobi operator of 9.
3
has discreteeigenvalues
111 112 ··· ~ ~.We
put E03BC = {V ~ 0393(N(M)); (V) = 03BCV}.
The number03A303BC0
dim(E03BC)
iscalled the index
of 9
or the index of M inN,
denotedby i(~)
ori(M).
Clearly, 9
is stable if andonly
if1(ç)
= 0. The number dim(Eo )
is calledthe
nullity
of ~ or thenullity
of M inN,
denotedby n(~)
orn(M).
A vectorfield V in
Eo
is called aJacobifield
of ~. We define asubspace
P ofT(N(M)) by
It is known that P c
Eo (cf. [S]).
We call the dimension of P theKilling nullity
of cp, denotedby nk(~)
ornk(M).
Here we
give
a lower bound for thenullity
ofcompact
minimal submani- folds inhomogeneous
Riemannian manifolds. Let N be an n-dimensionalhomogeneous
Riemannian manifold and M an m-dimensionalcompact
minimal submanifold immersed in N. LetI0(N)
be thelargest
connectedisometry
group of N and denoteby
g its Liealgebra,
thatis,
the Liealgebra
of all
Killing
vector fields on N. For x EN,
we denoteby Kx and x
theisotropy subgroup of Io (N )
at x and its Liealgebra, respectively.
We definea function a on M
by
for x E
M,
whereAV(X) = VN V (X E TX(N)).
Puta(M)
=Min {03B1(x);
l x E
M}.
For V E g and x EM,
we denoteby VTx (resp. VxN)
thecompornent of Vx tangent (resp. normal)
to M. Then weget
thefollowing.
PROPOSITION 1.1.
Proof.
We fix anypoint
x of M and define a linearmapping
IF: g ~Nx (M)
C Hom(Tx (M), Nx (M» by 03A8(V) = (VNx, ~~VNx).
Putg° = {V ~
g;VN
=0}
and we haveg°
c Ker(03A8).
Hence we havenk(M) =
dim
(g/g0) ~
dim(g/Ker (03A8))
= dim(Y’(g)).
Let{03BE1,
...,03BEn-m}
bean orthonormal basis for
Nx(M).
We chooseV03B1
E g(a
=1,
..., n -m)
so that
(VxN)x
=For
V Efx,
we have03A8(V) = (0, ~~ V"’)
andvi
VN =(VfVN)N = (~NXV - V VT)N = (~NXV)N - B(X, VT) = (AV(X))N
forX ~
Tx(M).
Hencelx
n KerCF) = {V ~ x; AV(Tx(M)) ~ Tx(M)}.
Thusdim
(P(fx))
= dim(ÏJ -
dim(î,
n Ker(03A8))
= dim(ÎJ - a(x).
Wetake a basis
{03A8(W1),
...,03A8(Wl)}
of03A8(x).
Then{03A8(V1),
...,03A8(Vn-m), P( »,;),
...,03A8(Wl)}
arelinearly independent.
Hence dim(03A8(g)) (n - m)
+ dim(’F(tx».
Thus weget nk(M) ~ (n - m)
+ dim(îj -
a(x). Q.E.D.
REMARK: The idea of this
proof
isinspired by
that of[S,
p.87].
2.
Homogeneous
vector bundles and Casimiroperators
In this section we recall some results from the
theory of homogeneous
vectorbundles.
Let G be a connected Lie group with the Lie
algebra
g and K a closedsubgroup
of G with the Liealgebra
f. We consider ahomogeneous
space M =G/K and
anatural principal
K-bundle 03C0: G ~ M. The coset K is calledthe
origin
of M and will be denotedby
o. For a finite dimensional rep- resentation(a, W)
ofK,
weget
aG-homogeneous
vector bundle(E
= G x(1 W, nE, M)
associated with theprincipal
bundle(G,
03C0,M).
All G-hom- ogeneous vector bundles over M are obtained in this fashion. We denoteby
i the action of G on E and M. Let
r(E)
be the vector space of all smooth sections of E on M. We denoteby
Coo(G; W)K
the vector space of all smooth W-valued functions on Gsatisfying f(uk)
=03C3(k-1)(f(u))
for u E G and160
k E K. G acts on
0393(E)
andCOO (G; W)K’ respectively, by
for 03BE
E0393(E), f ~ C~(G; W)K, g,
u E G and x E M. Forany 03BE
E0393(E)
wedefine
EC~(G; W)K by (03BE)03C0(u)
=u((u))
for u E G. The mapA: 1 - 1
ofT(E)
toC~(G; W)K
is a linearisomorphism preserving
the actions of G.For any
mapping
D:0393(E) ~ T(E),
we denoteby D
the map A · D -A-’ : C~(G; W)K ~ C~(G; W)K.
Assume that G is
compact
and(a, W )
is a finite dimensionalunitary representation
of K. Then E is acomplex
vector bundle with the hermitianfibre metric induced
by
the Hermitian innerproduct
of W. LetL2(E)
andL2(G; W)K
be thecompletion
of0393(E)
andC~(G; W)K
relative to theL2-inner products
inducedby
the normalized Haar measure of G and the Hermitian metric of E. Themap 03BE ~
extends to aunitary isomorphism
of
L2(E)
toL2(G; W)K preserving
the actions of G. LetD(G )
denotethe set of all
equivalence
classes of finite dimensional irreduciblecomplex representations
of G. Let for each 03BB ED(G), (o,,, V03BB)
be a fixedrepresenta-
tion of À. For each ED(G)
weassign
a mapAz from V.
(8)HomK V03BB, W)
to
C~(G; W)K by
the ruleA03BB(03C5
(8)L)(g)
=L(o03BB(g-1)03C5).
HereHomK (VÂI W)
denotes the space of all linear maps L
of V03BB
into W so thata(k) .
L = L - Qî(k)
for all k E K. For  E
D(G),
set039303BB(E)
=A-1(A03BB(V03BB
~HomK (V03BB, W))).
By
virtue of thePeter-Weyl
theorem and the Frobeniusreciprocity
thefollowing proposition
holds.PROPOSITION 2.1.
(cf. [Wa]): L2(E)
is theunitary
direct sum03A303BB~D(G)
Et)039303BB(E).
Moreover the
algebraic
direct sum03A303BB~D(G) 039303BB(E)
isuniformly
dense inr(E)
relative to the
uniform topology.
Let
( , )
be anad(G)-invariant
innerproduct
on the Liealgebra
g of G. We choose an orthonormal basis{X1,
... ,Xn
of g relative to( , ).
TheCasimir differential
operator
of G relative to( , )
is definedby
for f ~
COO(G).
Then we havePROPOSITION 2.2
(cf. [Wa]):
On each1-Â (E), W
is a constant operatoral/.
Herea is the
eigenvalue of
the Casimir operatorof
therepresentation Â
relative to( , ).
We do not suppose that G is
compact.
Let Tbe a connection in theprincipal
bundle
(G,
03C0,M, K)
which is invariantby
the left translations of G.0393 determines a
decomposition
g = f + m such thatad(K)m
= m(cf.
[K-N,I,
p.103]).
T induces the covariant differentiationV’
on E. For avector X on
M,
we denoteby
X* the horizontal lift of X to G relative to r.For 03BE
E0393(E)
and X E1-(T(M»,
we haveLet g
be a G-invariant Riemannian metric on M. Then g defines anad(K)-invariant
innerproduct Bm
on m. We denoteby
V the Riemannianconnection of g.
For X, Y,
Z E m, we haveHere
[X, Y]m
denotes them-compornent
of[X, Y]
in g.The
(rough) Laplacian
0394E relative toVE
is definedby
where
{ei}
is a local orthonormal frame field on M. Letan orthonormal basis of m relative to
Bm,
PROPOSITION 2.3.
If
G is compact, moregenerally unimodular,
thenProof
We fixpoints
x e M and u e G with x =03C0(u).
We define an ortho-normal frame field
{e1,..., em}
in aneighborhood
U of x so that(ei)uexp(tX)·o
=d03C4u · d03C4exp(tX)(Xi) = dj03C0(Xi)uexp(tX)
for i =1,
..., m, X E mand we have for any
By (2.2)
andad(K)m
= m we have for any Z E m,Hence we
get Em (~elei)x
= d03C0(03A3mi=1 trace (ad(Xi))(Xi)u).
SinceXl , ... , X,
are horizontal with
respect
tol,
weget (03A3mi=1 ~elei)*u
=Y-m (trace(ad (Xi))(Xi)u.
Pute* = 03A3mj=1 cjiXj,
where eachcji
is a smoothfunction on
03C0-1(U)
and for eachu ~ 03C0-1(U), (cji(u))
is anorthogonal
matrix. We
compute
Since
(e*i)u exp(tX) = (Xi)u exp(tX)
for any X E m, we havecji(u
exp(tX)) = 03B4ji.
Hence(Xcji)(u) =
0 for any X E m. Thus weget 03A3mi=1 e*i(e*i)(u) = 03A3mj=1 Xj(Xj)(u).
If G isunimodular,
then tracead(X) =
0 for any X E g.Q.E.D.
Suppose
that K iscompact.
We can extend B to anad(K)-invariant
innerproduct B
on g such thatB(, m) =
0. Let{Xm+1,
... ,Xl}
be an ortho-normal basis of relative to B. Then we
get
thefollowing.
COROLLARY 2.4:
Proof.
For anyinteger
a withn + 1 ~ a ~ m, 03BE ~ T(E)
and u EG,
wecompute
and
Hence
COROLLARY 2.5: Assume that G is compact and g is a Riemannian metric on
M induced
by
anad(G)-invariant
innerproduct ( , )
on g. Let W denote the Casimirdifferential
operatorof
G relative to( , ).
Then we haveREMARK: The
endomorphism 03A3l03B1=m+1 03C3(X03B1)2
coincides with the Casimiroperator
of therepresentation (a, W )
of K relative to( , ).
3. Jacobi
operator
oftotally geodesic
submanifolds incompact symmetric
spacesIn this section we
explain
a method fordetermining
thestability
ofcompact totally geodesic
submanifolds incompact symmetric
spaces. There seem to be inaccuracies in[C-L-N].
Here we reformulate this methodby using
resultsof Section 2.
Let N be a
compact
Riemanniansymmetric
space with the metric gN and M an m-dimensionalcompact totally geodesic
submanifold immersed in N.Then it is standard to show that the immersion ~: M - N is
expressed
asfollows: There are
compact symmetric pairs (U, L)
and(G, K)
with N =U/L
and M =G/K
so thatwhere Q: G - U is an
analytic homomorphism
witho(K)
c L and theinjective
differential Q: g - u which satisfieso(m)
c p. Here u = 1 + p and g = f + m are the canonicaldecompositions
of u and g,respectively.
Denote
by
03B8 the involutiveautomorphism
of thesymmetric pair (U, L).
Wechoose an
ad(U)-invariant
innerproduct ( , )
on u such that( , )
inducesgv. We also denote
by ( , )
thead(G)-invariant
innerproduct
on g induced from( , ) through
Q. Let g be the G-invariant Riemannian metric on M inducedby ( , ).
Then (p:(M, g) ~ (N, gN)
is an isometric immersion. LetN(M)
be the normal bundle of ç and denoteby T(N(M))
the vector space of all smooth sectionsof N(M)
on M. We canidentify p,
m ando(m)
withTo(N), To(M)
and~*(To(M)), respectively.
Letml
be theorthogonal compliment
ofQ(m) with p
relative to( , ).
Weidentify m~
withNo(M).
Define an
orthogonal representation
6 of K on m~by 03C3(k)(03C5)
=ad(o(k))03C5
for k E K and v E ml . The normal bundle
N (M)
is thehomogeneous
vectorbundle G x
03C3m~
over M associated with theprincipal
K-bundle 7c: G - M.As in Section 1 there is a linear
isomorphism 0393(N(M)) ~ Coo(G; m~)K;
V -
V. Let {X1,
... ,XI
be an orthonormal basis relative to( , )
suchthat
IXI,
... ,Xm}
is in m and{Xm+1, .XII
is in . Let W be the Casimir differentialoperator
of G relative to( , ).
Let
Fo
be the canonical connection of n: G ~G/K
andV’
the covariant differentiation of G x03C3m~
induced fromro.
We denoteby A’
the(rough) Laplacian
defined fromV’
and the Riemannian connection Vof (M, g).
LetV.l be the normal connection of 9 on
N (M)
and dl the(rough) Laplacian
defined from
~~
and V. Since cp istotally geodesic,
we have thefollowing.
PROPOSITION 3.1:
Vo
=~~.
By Corollary
2.5 andProposition 3.1,
weget
Let
f1-
be theorthogonal complement
ofe (f)
in 1 relative to( , )
andput
g1- = ~
+m1.
Then the vector spaceg1
isad(o(g))-invariant
and we havean
orthogonal decomposition
u =o(g)
+g1
asad(o(G))-modules.
Wedenote
by (03BC, g1)
thisrepresentation
of G ong1- .
The Casimiroperator
of therepresentation p
relative to( , )
isgiven by C03BC
=£5=1 ad(o(XA))2
EEnd(g~).
Then the Jacobioperator 3 of ç
isexpressed
in terms of W andC,
as follows:
LEMMA 3.2:
Proof.
Since ç istotally geodesic,
wehave = - 0394~
+R~.
As thecurvature tensor
RN
of asymmetric
space N isgiven by RN (X, Y)Z
=-
[[X, Y], Z]
forX, Y,
Z E m, we havefor V E
0393(N(M))
and u E G. Hencewe get
There is an
orthogonal decomposition gl
=g j
~ ··· E9gk
such thateach
g’
is an irreduciblead(o))(G-invariant subspace
with0(gl) = gt.
.Then
by
Schur’s lemma we haveCu - ail
on eachgt.
Here ai is theeigenvalue
for the Casimiroperator
of the irreducible G-moduleg’
relativeto
( , ).
Putg~i = ~i
+m/ ,
wheret-’ =
~ ngi
andm’ = ml
ngl
.166
Then we have
ad (o(K))~i
=ff
andad(o(K))m~i = mf.
Denoteby (ui, mf)
this
representation
of K onm~i.
Thedecomposition
m~ =mi O ’ ’ ’
Qm-’
induces the
decompositions
and
By
Lemma 3.2 we have forTHEOREM 3.3: The
index, nullity
andKilling nullity of
qJ aregiven as follows:
where
m(Â)
=dim’H-- (m~i)C)
anddÂ
denotes the dimensionof
therepresentation
À.4.
Stability
ofHelgason spheres
Let
(N, gN)
be an n-dimensionalcompact
irreducible Riemanniansymmetric
space and
Io(N)
thelargest
connected Lie group of isometries of N. Let Kbe the maximum of the sectional curvatures of N.
By
a theorem of E.Cartan,
the same dimensional
totally geodesic
submanifolds of N of constant cur- vature 0 are allconjugate
underIo(N). Helgason proved
ananalogous
statement for the
maximum
curvature K as follows.THEOREM 4.1
([H1]):
The space N containstotally geodesic submanifolds of
constant curvature K.
Any
two suchsubmanifolds of
the same dimensionare
conjugate
underIo(N).
The maximal dimensionof
suchsubmanifolds
is1 +
m(ô)
wherem(ô)
is .themultiplicity of
thehighest
restricted root ô.Also,
K =
4n21b12, where 1 1
denoteslength. Except for
the case when N is a realprojective
space, thesubmanifolds
aboveof
dimension 1 +m(ô)
areactually spheres.
Assume
that
N is not a realprojective
space. LetSK
be a maximal dimension- altotally geodesic sphere
of N with constant curvature K. We callSK
theHelgason sphere
of N. In this section we show that everyHelgason sphere
is a stable minimal submanifold of N. Put m = 1 +
m(ô).
We
begin
withpreliminaries
on Liealgebras.
Let(U, L)
be acompact symmetric pair
with N =U/L.
Let u and 1 be the Liealgebras
of U andL, respectively,
and u = 1 + p the canonicaldecomposition.
We choose thead(U)-invariant
innerproduct ( , )
on u so that( , )
induces gN. Let a bea maximal abelian
subspace of p
and t the maximal abeliansubalgebra
ofu
containing
a. We denoteby
UC thecomplexification
of u. For a Et,
wedefine a
subspace
ofu’ by
a E t is called a root of u with
respect
to t if oc *- 0 and03B1 ~ {0}.
We denoteby 03A3(U)
thecomplete
set of roots of with to t. Thefollowing proposition
is well known
(cf. [H2]).
PROPOSITION 4.2:
(1)
For a E03A3(U),
we have dimû« -
1.(2) ûo - tC.
(3)
There is a direct sumuc
=tc
+L(xEI(U) U(X’
called the rootdecomposition of uc
with respect to t.(4)
For a,f3
Et,
we have[û«, ûfll
c03B1+03B2.
Inparticular, if
a,f3,
a +f3
El(U),
we have[û«, 03B2] = 03B1+03B2.
For y E a, we define a
subspace
ofuc by
y E a is called a root of
(u, 1) (or
a restricted root ofu)
withrespect
to a if:0 0 and u’ *
0. We denote bel(U, L)
thecomplete
set of rootsof (u, 1).
We have a direct sum
u’
=u’
+03A303B3~03A3(U,L) uC03B3,
and[u’, uC03B4] ~ uC03B3+03B4.
Wehave a direct sum t = b + a, where b = t n 1. We
put 4(U) l(U)
n b.We define an involotive
automorphism
of t asa(H1
+H2 ) - - Hl
+H2
for
Hl
E b andH2 ET a.
A linear order of t is called a a-order if for any03B1 ~ 03A3(U) - 10 (U) with a
>0 we have 03C3(03B1)
> 0.There always is 03C3-order
of t. We fix a 03C3-order . We denote
by
1+( U )
and 1+( U, L)
thecomplete
sets of
positive
roots of u and(u, 1), respectively.
For H Et,
we denoteby
FI
thea-compornent
of H withrespect
to( , ).
Then we have I+(U, L) =
{03B1;
a EI+ (U) - 03A30(U)}. For y
E a, weput
168 and
The
following propositions
are well known(cf. [H2], [Te2]).
PROPOSITION 4.3:
(1)
We haveorthogonal
direct sumsof
1and p
relative to( , );
For each y E
03A3+(U, L),
we have dimI03B3
= dimPY’
denotedby m(y).
(2)
For y El(U, L),
we haveand
and
PROPOSITION 4.4: For each a E 03A3+
(U) - 03A30(U),
we can chooseSa
E1, Ta
E psatisfying the following properties:
are orthonormal bases
of Iy
andp03B3, respectively.
and
for any H E a.
Assume that
(U, L)
is irreducible and N is not of constant curvature. LetÔu
be the
highest
root of E+(U). Then 03B4 = 03B4U
is thehighest
root of Il(U, L)
and the maximum of the sectional curvatures of
(N, gN)
is403C02|03B4|2.
PROPOSITION 4.5 we have
PROPOSITION 4.6
(cf. [Hl]): spanR{03B4}
+ m is a Lietriple
systemof (U, L)
which generates a maximal
totally geodesic sphere SK of
constant curvature K =4n21b12.
Set
and
Note that set
and
Then we have
and
Here
1(1)
=Ib and p(1)
= pb.Let G be an
analytic subgroup
of Ugenerated by
the Liealgebra
g and K ananalytic subgroup
of Lgenerated by
the Liealgebra
f.Then Sx
isexpressed
as ahomogeneous
spaceG/K
associated with thesymmetric pair
(G, K).
170
We denote
by fo
theorthogonal complement of[pb’ pa in I0
relative to theinner
product ( , )
andput ô’ = {H
E a;(b, H) = 0}.
Then we haveand
Under the identification we have
It is clear that
(ad
We prepare some
propositions.
PROPOSITION 4.7:
Proof. By Proposition z
withand
And we have
and
PROPOSITION 4.8:
Proof. Using Proposition
4.3(3)
wecompute
and
PROPOSITION 4.9:
Proof. Using Proposition
4.3(3),
wecompute
and
Combining Propositions 4.7,
4.8 and4.9,
we obtain thefollowing.
LEMMA 4.10:
Note that is
an orthonormal basis
of 1
from
Proposition
4.6 we havePROPOSITION 4.11:
and
for any real number t. In
particular
weget
and
173
We put Then
by
Lemma 4.10 for
we
compute
and
Let Then there is
an element
we have
Therefore
by
Lemma 4.10 we haveSet
and
PROPOSITION 4.12: The
index, nullity
andkilling nullity of SK
aregiven
asfollows;
where
m(À)
= dimHom,
Proof. By
Lemma 4.11 the Casimiroperator
of therepresentation (ad, g~0)
of G relative to
( , )
is a zerooperator.
It follows fromProposition
4.11 thatHence the Casimir
operator
of therepresentation (ad, gt)
of G relative to( , )
is the constantoperator - (m(m
+1)/2)03C02|03B4|2I.
Thus from Theorem3.3 we
get (1), (2)
and(3).
THEOREM 4.13
Proof. Set
Proposition
4.12 weget
In each case g and t are
given
as follows(cf.
Table1):
(1)
If N is a groupmanifold,
then(2)
If N is oftype All,
then g : =Table 1.
Here m = 1 + m(03B4); 03BA =
4n’lôl’
and p = card{03B1
E E(U); ± 2(03B1, 03B4) = (03B4,03B4)}.
Eachcompact irreducible symmetric space N = U/L is equipped with the invariant Riemannian metric induced by the Killing-Cartan form of the Lie algebra of U.
By
the formula of Freudenthal(cf. [Te2])
we can determine theeigenvalues
of Casimir
operators.
Forexample,
theeigenvalues
of Casimiroperators
176
relative to the
Killing-Cartan
metric aregiven
asfollows;
By examining
theeigenvalues
of Casimiroperators
caseby
case, we obtainthe
following:
177
By
the directcomputations
we obtainAccording
to the tables for thebranching
rules in[M-P]
we have thefollowing.
178
Hence we
get
and
Thus we obtain
i (SK)
= 0. Thedecomposition
of each(gt)C
as a G-modulein each case is
given
as follows:(1)
If N is a groupmanifold,
(2)
If N is oftype AII,
(3)
If N is oftype CII,
(4)
If N is oftype
EIV(5)
If N is oftype FII,
(6)
If N isotherwise,
Therefore
by Proposition
179 REMARK:
and
From our result and the second variational formula for a harmonic map we
immediately
see that if m =2,
the inclusion mapl : S03BA ~
N is also stableas a harmonic map.
(2) By introducing
a calibrationby
the fundamental 3-form onsimple
Liegroups, Tasaki
[Ts] proved
that if N is a groupmanifold, then S03BA
is homo-logically
volumeminimizing
in its realhomology
class.5. A remark on certain submanifolds associated with
Helgason spheres
Here we show a
generalization
ofProposition
3.8 in[01,
p.214]
andLemma 5 in
[O-T,
p.13].
LetG(m, N) = ~x~N G(m, Tx(N))
be the Grass-mann bundle of all nonoriented
m-planes
on an irreduciblesymmetric
space N. Setjo
=spanR{03B4}
+ m. c m =To(N)
and m = dim03BE0.
Now wedefine a
subbundle .5
ofG(m, N) by
An m-dimensional submanifold M of N is called an
b-submanifold
if everytangent
space of Mbelongs
tob.
Forexample,
in case that M is a Hermitiansymmetric
space, anb-submanifold
is a 2-dimensionalcomplex
submani-fold. In case N =
P2(Cay),
anb-submanifold
is aCayley
submanifold(cf.
[01],
and in case that N is asimple
Lie group, anb-submanifold
is a~-submanifold,
thatis,
a calibrated submanifold associated with the cali- bration definedby
the fundamental3-form cp
of the Lie group N(cf. [Ts], [O-T]).
In[O1]
and[O-T]
we showed that aCayley
submanifold and(p-submanifold
aretotally geodesic.
Thefollowing generalizes
theirs.PROPOSITION 5.1: Let M be an
b-submanifold of
N. Then M is a minimalsubmanifold of
N. Moreoverif
m = dim M >3,
M is atotally geodesic
submanifold of
N.We prepare a lemma in order to show the above
proposition.
LEMMA 5.2: Let N be a
locally symmetric
space and M a curvature-invariantsubmanifold of N,
that is,RN(X, Y)Z
ETx(M) for
any x E M and anyX, Y,
Z E
Tx(M).
Here we denoteby
RN and B the curvature tensorof
N andthe second
fundamental form of M, respectively.
Thenfor
any vectorsX,
Y ETx(M)
we haveProof. RN and B satisfy
anequation
that
and
Adding
these twoequations,
weget
the desiredequation. Q.E.D.
Proof of Proposition
5.1. We fix anypoint
x E M. We canidentify Tx(M)
and
Tx(N)
with03BE0 and p, respectively.We regard
the second fundamental form B as asymmetric
bilinear form B :Ço
x03BE0
~03BE~0, where j)
denotes theorthogonal complement
of03BE0
in p. For any orthonormal vectorsX,
Y E03BE0,
by RN (X, Y)Y
= KX and Lemma5.2,
we haveSince
{03B41
=ô/lôl, T(X; II
E03A3+(U) - 03A30(U), 03B1 = bl
is an orthonormal basis ofÇo, transforming
itby
anisometry
ofN,
if necessary, we may assume that X =ô,
and Y =7,. As j)
= 03B4~ +p(0)
+p(1/2),
we denoteby B’
and B" the
(03B4~
+p(0))-
andp(1/2)-components
ofB, respectively. By Lemma 4.10 we have (ad X)2 B’ = (ad Y)2B’ = 0. By Proposition
4.11 wehave
(ad X)2B" = -03C02|03B4|2 B"
and(ad Y)2B" = -(1/4)03BAB".
By
Lemma 4.10 we haveFor any , we
compute
and
Hence we
get
Since we have
Hence we
get ((ad Y)(ad X)
+(ad X)(ad Y)) p(1/2) = {0}.
Thus((ad Y)(ad X)
+(ad Y) (ad X)) B(X, Y)
= 0. Therefore(5.1)
becomes182
It follows from this that
B (X, X)
+B( Y, Y)
= 0 for any orthonormalvectors
X,
Ytangent
to M.Q.E.D.
6. Indices and nullities for
totally geodesic
submanifolds incompact
rankone
symmetric
spacesUsing
our method we can determine theindices,
the nullities and theKilling
nullities of all
compact totally geodesic
submanifolds incompact
rank onesymmetric
spaces. In[01]
we stated these resultspartially.
In this section wegive
theircomplete
table.PROPOSITION 6.1: The index and the
nullity of
each compacttotally geodesic submanifold
M in a compact rank onesymmetric
space N aregiven
as inTable 2. In each case the
nullity
isequal
to theKilling nullity.
REMARK:
(1)
The results of N = S" and N =Pn(C)
were shownby
Simons[S]
and Kimura[K], respectively.
See also[Te3].
(2)
Simons[S]
showed that agreat sphere
S"’ of S" is aunique
m-dimensional
compact
minimal submanifold of S" with the lowest index and the lowestnullity.
Kimura[K]
showed that acomplex projective
sub-space
P,(C)
ofPn(C)
is aunique
m-dimensionalcompact
minimal sub- manifold ofPn(C)
with the lowestnullity.
These results for thenullity
areTable 2.
generalized
as follows. LetF,
F’ =R, C,
UD orCay.
We denoteby Pn(F)
ann-dimensional
projective
space over F. Here n = 1 or 2 when F =Cay.
Suppose
that F’ ce F andPm(IF’)
is aprojective subspace of Pn(F).
We fix apoint o
EPm(F’).
We call that a submanifold M ofPn(F)
is of typePm (F’)
if for
any ,,
E M there is anisometry
i ofPn(F)
such thatTx(M) = (d03C4)o(To(Pm(F’))). Clearly, Pm(F’)
is a submanifold oftype Pm(F’).
Forexample,
if F = Cand
F’ =C,
then a submanifold oftype Pm (IF’)
is acomplex
submanifoldof Pn(C).
If F = C and F’ =R,
then a submanifold oftype Pm(F’)
is atotally
real submanifold ofPn(C). Using
the method ofProposition
1.1 we canshow
thefollowing.
Let M be acompact
minimal submanifold oftype Pm(1t:’)
immersed inPn(F)
and denoteby
cp its immer- sion. Thenn(~) ~ nk(~) ~ n(Pm(F")). Moreover, nk(cp)
=n(Pm(F’))
if andonly
ifcp(M)
iscongruent
toPm(IF’).
(3)
An m-dimensional realprojective subspace Pm(R)
ofPn(C)
is notalways
atotally
realcompact
minimal submanifold with the lowest index.In
fact,
thetotally
realcompact
submanifold M =SU(3)/SO(3). 7L2
embedded in
P5(C) (cf. [N])
hasi(M)
=8(
15 =i(P5(R))
andn(M) = nk(M)
= 27. It seems that every n-dimensionaltotally
realcompact
minimal submanifold M embedded inPn(C)
with theparallel
second fundamental form hasi(M)
=dim I0(M)
andn(M)
=nk (M)
=dim I0(Pn(C)) -
dim
I0(M).
7.
Instability
of rectifiable currents oncompact symmetric
spacesIn this section we show an
instability
theorem for rectifiable currents oncompact
minimal submanifolds in asphere.
Moreoverusing
our result andthe first standard minimal immersions of
compact
irreduciblesymmetric
spaces, we show a nonexistence theorem for rectifiable stable currents of certain
degrees
on somecompact symmetric
spaces.Let N be an n-dimensional
compact
Riemannian manifoldand Rp(N, A)
the group of rectifiable
p-currents
on N overA,
where A is afinitely generated
abelian group. We denoteby JP(N, A)
the group ofintegral
p-currents
on N over A.THEOREM 7.1
(Federer
andFleming [F-F], Fleming [FI]):
There is a naturalisomorphism of
thehomology
groupsH*(f*(N, A))
with thesingular
homol-ogy groups
H*(N, A).
THEOREM 7.2
(Federer
andFleming [F-F], Fleming [Fl]):
For every nonzerohomology
class a EHp(F*(N, A)) - HP(N, A)
there is a F E aof
at leastmass in the sense that 0
M(F) ~ M(F’) for
all F’ E a.184
An element F E
RP(N, A)
is called stable if for every smooth vector field Von N with the flow (p, there is an 03B5 > 0 such that
M(~t*F) ~ M(F)
for all|t|
03B5.THE GENERALIZED PRINCIPLE OF SYNGE
If there
are no nonzero stable currents inRp(N, A),
thenHP(N, A) = {0}. If
p = 1 and A =
Z,
then notonly
doesH1(N, Z)
={0}
but N is alsosimply
connected.
If
p = 2 and A =7L,
then notonly
doesH2(N, 7L)
={0}
butn2 (N) = {0}.
This is due to Theorem 1 and
2,
the classical result of closedgeodesics
andthe theorem of Sacks-Uhlenbeck for the existence of stable minimal
2-spheres (cf. [S-U]).
Let ç E 039BpTx(N) be a
unitsimple p-vector.
For any vector field V on Nwith the flow ~t, we define a quadratic form Q03BE by Q03BE (V) = (d2/dt2)|~t*03BE||t=0.
For
any F
EPllp(N, A),
we define aquadratic
formQF by QF(V) = (d2/dt2)M(~t*F)|t=0.
Then we haveQF(V) = J Qyx(V) d~F~ (cf. [Fe]).
Now assume that N is
isometrically
immersed in a Euclidean space (EN and does not lie in any properhyperplane
ofEN.
Weput 1/ = {grad f03C5
E0393(T(N)); 03C5
EEN},
wheref03C5(x) = ~x, 03C5~
for x E N. There is a naturalisomorphism V ~
(EN. Then the trace ofQ03BE
on V withrespect
to the innerproduct
induced fromEN
isgiven
asfollows;
PROPOSITION 7.3
(cf. [01]):
where B denotes the
second fundamental form of N
andnq}
is an orthonormal basisDenote
by
R the curvature tensor of N and define the sectional curvatureof N as
K(X
039BY) = R(X, Y)Y, X ~/~ X
039BY~2.
The Ricci tensor of Nis defined
by
Ric(X, Y)
=03A3ni = 1 ~R(X, ei)ei, Y),
where{ei}
is an ortho-normal basis of
Tx(N).
The mean curvaturevector 1
of N is definedby
q =
(1/n)03A3ni=1 B(e;, ei).
Theequation
of Gauss isgiven
asfollows;
Put. We use the
following
convention on the range ofindices;
185 Then we
compute
By
theequation
of Gauss weget
If N is a submanifold of a
hypersphere SN-1(r)
with theradius r, (7, 1)
becomes
where B8 denotes the second fundamental form of N in SN-1
(r).
Furthersuppose that N is a minimal submanifold of