1547845447-The_Ricci_Flow_-_Techniques_and_Applications_-_Part_IV__Chow_

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164 30. TYPE I SINGULARITIES AND ANCIENT SOLUTIONS

Then by (30.109) we have

so that \79^00 (tlm 00 (t) is a parallel gradient vector field.
Claim.

(30.116) v~ (t) = v;; (t).


Proof of claim. (1) m 00 (t) is constant. Then \79^00 (tJet, (t) = \79^00 (t)g~ (t) and


6. 900 (t)et, (t) = 6. 900 ctJR~ (t). In this case, (30.111) implies et, (t) = e~ (t), which


in turn yields (30.116).
(2) m 00 (t) is not constant. Then \79^00 (tlm 00 (t) is nonzero and by the de Rham

holonomy splitting theorem we have the following. The shrinker (M 00 ,g 00 (t)) is


isometric to (Nn-^1 ,h(t)) x (IR,ds^2 ) , where (N, h(t)) is isometric to {x E M 00 :


m 00 (x, t) = O} with the metric induced by g 00 (t). Moreover, there exist a, b E IR


depending on t with a -=/=- 0 such that

(30.117) m 00 (y, s , t) =as+ b


for y EN and s ER From (30.109) we can now show that there exists ¢(t) : N-+ IR
such that
s2 A

e~ (y, s , t) = ¢ (y, t) - - +as+ b


4t

(

s )2 A


= ¢ (y, t) -


2

t - at + b + a^2 t^2


for some a, b E IR and


By translating the coordinate on IR and absorbing the constant b + a^2 t^2 into ¢ , we


may assume that a = b = O; i.e.,


s2

e~ (y, s, t) = ¢ (y, t) -


4

t.


Hence, by (30.112) and (30.117), we have

This implies


o = Iv e;t, ( t) 12 + et,t ( t) - Ive~ ( t) 12 - e~/ t)


I a) 2 as+ b
= 2a \ ve~ (t)' OS +a + -t-

b
= a2 + -.
t

moo (y, s, t) =as - a^2 t.

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