1547845447-The_Ricci_Flow_-_Techniques_and_Applications_-_Part_IV__Chow_

(jair2018) #1
96 29. COMPACT 2-DIMENSIONAL ANCIENT SOLUTIONS

LEMMA 29.29. There exists a constant c 1 > 0 such that for all t E (-oo, -1],


(29.85) c1^1 itl :::; Pt :::; C1 itl ·


Hence diam(g(t)):::; Cltl.


PROOF. STEP l. There exists a constant C < oo such that for each t ,
(29.86) c-^1 pt :::; Pt:::; Cpi.
Since Lg(t) ht):::; C by (29.66), we h ave

(29.87) diam(g(t)):::; Pt+ Pt+ C.


Since B^9 x, ~) (pt) c S~Jt) and by Lemma 29.23, there exists a constant c > 0


such that for all t ,

c < A ±ht)



  • A =Fht)
    Area 9 (t)(B!~\Pt +Pt+ C) - B!~)(pi))


< l l


Areag(t) (Bx,^9 ~) (p'i))

< (Pt+ Pt+ C)^2 - (/[')^2


(pi)2
by the relative Bishop- Gromov volume comparison theorem. The above inequality
says that
v'C+Ipi :::; Pt + Pt + C.

Hence Pi :::; C Pt for some constant C < oo.


STEP 2. Bounds for Pt. By (29.79) and (29.82), we have Pt :::; ~~ ltl.


By (29.87) and the relative Bishop- Gromov volume comparison theorem, we
have

Area g(t )(Bg(t)(p'f) xi t - Bg(xi t)(p'f t - 1))


Areag(t)(Bxg~)(Pt +Pt+ C) - Bx^9 ~\p't))
< l .,


  • Area g(t) (Bg(txi )(p'f)-Bgt xi (t)(p'f-l)) t


< (Pt+ Pt+ C)^2 - (pi)^2


(/[')2 - (/! - 1 )2


:::; Cpt


by (29.86).
From the geometry of t he neck we obtain


(29.88) Area 9 (t)(B^9 xt ~)(pt) - B^9 xt ~)(Pt - 1)):::; C.

Hence


(29.89)

where the last inequality follows from (29.72). This completes the proof of the
lemma. O

Free download pdf