1547845440-The_Ricci_Flow_-_Techniques_and_Applications_-_Part_III__Chow_

(jair2018) #1

  1. MEAN VALUE INEQUALITY FOR SOLUTIONS OF HEAT EQUATIONS 313


Note that
87/Ji 2i 2i+l
(25.32) 0 < - < - and l\77/Jilg-S -.

- ar - T5 To


Here \77/Ji is a C^00 vector field on the complement of the cut locus of xo (the
cut locus is a closed set with measure zero).
We then have

supp('t/Ji) C Pri' 7/Ji = 1 on Pri+i"


Moreover, by (25.32) and 7/Ji :::; 1, we have

(25.33) 7/Ji ~~i + l\77/Jil~ S 4i+^2 T 02 ~Li.


Now we may take 'ljJ = 7/Ji in Step 2.


Corresponding to (25.27), define
(25.34)

M· ='= ecs(i+v.Kri) ((1+1)2 cn+14i+2 + 1) (2cn4i+2T-2) ~
i • Vol2/n ( ) 2i-1 0 0 0 ·
9 B_g xo, Ti
By (25.28), with T =Ti, T^1 = Ti+l, p =Pi, and M =Mi, we have (note that
Pi+l = n~^2 Pi)
n 1
llvllL^2 Pi+l(Pri+i) S Mt+


2 2
Pi llvllL2Pi(Pri)'

where we used the fact that Ti :::; 2To and (25.8) imply B (xo, 4To) c D.


Hence, for any integer j 2 2

llvllL"'; ( P.,) :S ()j M,.:;,,;,) llv llv (P.>c,) ·


Taking the limit as j-+ oo, we have


llvllL-(P.,) :S (Il M;~' ,;, ) llvllL'(P,.,)


(25.35)

where
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