1547845440-The_Ricci_Flow_-_Techniques_and_Applications_-_Part_III__Chow_

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then


  1. HEAT KERNEL FOR STATIC METRICS


det M ( 8) = 1 + 8 · tr (A) + 8^2 (tr ( B) + t tr^2 (A) - t tr (A^2 ))


+ 83 ( tr (A) ( ~ tr^2 (A) - ~ tr ( (A)


2
) + tr ( B)) )

+ ~ tr ( (A)^3 ) - tr (AB) + tr ( C)


+0(8^4 ).


Moreover, if A = 0, then


(23.139) det M (8) = 1+8^2 tr (B) + 83 tr (C)



  • 8^4 (ttr^2 (B) -t tr (B^2 ) +tr (D)) + 0 (8^5 ).


PROOF. Recall that if M = M ( 8) is a time-dependent invertible matrix,
then

(23.140) ds d detM = detM ·tr ( M-^1 dM) d
8 ,

so that if Mis given by (23.138), then


: 8 's=O detM =tr ( d:).


Differentiating (23.140), we have
(23.141)

d

2
det M = det M · (tr^2 (M-^1 dM) -tr (M-^1 dM M-^1 dM))
~ ~ ~ ~

(

+ det M · tr M -1d2M) d


82 ,

so that if Mis given by (23.138), then


We compute
(23.142)

:: 2 1s=O det M = (tr


2

(A) - tr (A


2
) + 2 tr (B)).
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