Isoparametric Submanifolds and Their Focal Manifolds 165
We start with the first possibility. We can assume, by considering a neighborhood
of p if necessary, that all local orbits of Φ
¯p
in S(p) have the same dimension. Since
the integral manifolds S(x) move by parallel transport in the normal bundle of M
ξ
,
we can assume that the local orbit Φ
¯q
·q in S(q) is of maximal dimension for any
q ∈ M. In this way we obtain a distribution
˜
ν
on M given by the normal space
˜
ν
(q)
in S(q) of the orbit Φ
¯q
·q. Note that
˜
ν
(q)
⊥
is the tangent space of the holonomy
tube (M
ξ
)
−
ξ
(q)
⊂M at q. We will show that the distribution
˜
ν
satisfies the cond ition
of Moore’s Lemma 1.7.1, which then implies
˜
ν
= 0sinceM is locally irreducible
(
˜
ν
= TM,otherwise
ξ
would be umbilical) . The distribution
˜
ν
is autoparallel by
the Normal Holonomy Theorem and Proposition 2.3.11. By the proof of Proposition
2.3.11, if p
2
∈ L (p
1
),whereL (p
1
) denotes the integral manifold of
˜
ν
through p
1
,
then
η
p
1
= p
2
− p
1
belongs to the normal space of Φ
¯p
1
· p
1
at p
1
(regarded as a
submanifold of the affine normal space ¯p
1
+
ν
¯p
1
M
ξ
). If p
2
is close to p
1
then
η
p
1
is
fixed by the isotropy subgroup of Φ
¯p
1
at p
1
,sinceΦ
¯p
1
·p
1
and Φ
¯p
1
·p
2
have the same
dimension (note that ¯p
1
= ¯p
2
,sinceL (p
1
) ⊂ S(p
1
)). By Proposition 2 .3.5 (see also
Remark 2.3.10)
η
p
1
extends to a Φ
¯p
1
-invariant and ∇
⊥
-parallel normal vector field
on the orbit Φ
¯p
1
.p
1
in ¯p
1
+
ν
¯p
1
M
ξ
. It is now standard to show that
η
p
1
extends to a
parallel normal vector field
η
on the holonomy tube (M
ξ
)
−
ξ
(p
1
)
. Thus (M
ξ
)
−
ξ
(p
2
)
coincides with the parallel manifold ((M
ξ
)
−
ξ
(p
1
)
)
η
to (M
ξ
)
−
ξ
(p
1
)
.
Note that the distribution
˜
ν
consists of fixed points of the isotropy group of Φ
¯q
at q. Considering horizontal and vertical curves and applying similar arguments as in
Section 4.4.4, we obtain that
˜
ν
defines by restriction a ∇
⊥
-parallel flat subbundle of
the normal bundle of any holonomy tube (M
ξ
)
−
ξ
(q)
(regarded as a submanifold of the
ambient space). Moreover x +
η
(x) belongs to the leaf L (x) for any x ∈ (M
ξ
)
−
ξ
(q)
.
Let A, A
1
, A
2
and
¯
A be the shape operators of M, (M
ξ
)
−
ξ
(p
1
)
, (M
ξ
)
−
ξ
(p
2
)
and M
ξ
respectively. If H is the distribution given by the horizontal spaces of the holonomy
tubes (M
ξ
)
−
ξ
(q)
⊂ M (q ∈ M), then H (p
1
)=T
¯p
1
M
ξ
= H (p
2
), regarded as sub-
spaces of R
n
. Note that H = E
⊥
. The distribution H is invariant under the shape
operators of M and of the holonomy tubes. The restriction of
ξ
to any holonomy tube
(M
ξ
)
−
ξ
(q)
⊂ M, q ∈ M, is also a parallel normal vector field on this submanifold of
R
n
. This is a consequence of the invariance of H under shape the operators of M
and of the holonomy tube and the fact that A|
H
⊥
= id. Moreover, A
1
ξ
(p
1
)
and A
2
ξ
(p
2
)
have the same eigenvalues as A
ξ
(which are constant), with the possible exception of
1if
˜
ν
= ker(id −A
ξ
). This implies A
1
ξ
(p
1
)
= A
2
ξ
(p
2
)
if
η
is sufficiently close to 0. In
fact, both shape operators are simultaneously diagonalizable by the “tube formula”.
Note that
ξ
(p
i
)= ¯p
i
− p
i
, i = 1,2, so
ξ
(p
2
)=
ξ
(p
1
) −
η
(p
1
). By Lemma 4.5.5 we
have A
1
η
|
H
= 0, since H = E
⊥
=(ker(id −A
ξ
))
⊥
=(ker(id −A
1
ξ
))
⊥
(the distribu-
tions are restricted to (M
ξ
)
−
ξ
(p
1
)
). Thus
η
is constant along horizontal curves (with
respect to H ). But any two points in (M
ξ
)
−
ξ
(p
1
)
can be joined by a horizontal curve
(by the construction of the holonomy tube), so
η
is constant along (M
ξ
)
−
ξ
(p
1
)
in R
n
.
Therefore, the leaves of the autoparallel distribution
˜
ν
are parallel in R
n
along
any holonomy tube (M
ξ
)
−
ξ
(q)
.Since
˜
ν
⊥
is the distribution tangent to the holonomy
tubes,
α
(
˜
ν
,
˜
ν
⊥
)=0, where
α
is the second fundamental form of M.Furthermore,
˜
ν
is a parallel distribution on M, as it is autop a rallel and its leaves are parallel (in R
n
)