- NECKLIKE POINTS IN ANCIENT SOLUTIONS 271
On the other hand, if .A (T - t) 2: c, then μ^2 + v^2 > 8.\^2 and we have
d c 1 - c 8.\^2
- log < c;,A - - -- < 0
dt 2 (T - t) 2 .A+μ + v + p -
for c; > 0 small enough. D
- Necklike points in ancient solutions
The objective of this section is to show that an ancient solution of posi-
tive sectional curvature is either isometric to a spherical space form or else
contains points at arbitrarily ancient times where its geometry is arbitrarily
close to the product of a surface and a line. We begin with some general
observations about ancient solutions - including the fact that every ancient
solution (of any dimension) has nonnegative scalar curvature.
LEMMA 9.15. Let (Mn, g (t)) be a complete ancient solution of the Ricci
flow. Assume that Rmin (t) ~ infxEMn R (x, t) is finite for all t :S: 0 and that
there is a continuous function K (t) such that !sect [g (t)]I :S: K (t). Then
g (t) has nonnegative scalar curvature for as long as it exists.
PROOF. Recall that the parabolic maximum principle works on noncom-
pact as well as on compact rpanifolds. Recall also that
~~ = b.R + 2 IRcl
2
2: b.R + ~R
2
.
So if R ever becomes nonnegative, it remains so for as long as the solution
exists. On the other hand, if Rmin (t1) < 0, then Rmin (to) < 0 for all to :S: ti,
and one has
n n
Rmin (t) > 1 > ----
- n (Rmin (to))- - 2 (t - to) - 2 (t - to)
for all t > t 0. Since the solution is ancient, we may let to ""' - oo, obtaining
Rmin (t) 2: - lim ( n ) = 0.
to->- oo 2 t - to
D
REMARK 9.16. In dimension n = 3, we can strengthen this result, as we
proved in Corollary 9.8.
In Lemma 8.19, we derived a lower bound for the blow-up rate of so-
lutions that develop singularities in finite time. The analogous result for
ancient solutions is the following:
LEMMA 9.17. Let (Mn, g (t)) be an ancient solution with nonnegative
Ricci curvature. Then there exists a constant co > 0 depending only on n
such that
liminf ltl sup IRm (x, t)I 2: CO·
t->- oo xEMn