134 5. THE RICCI FLOW ON SURFACES
PROPOSITION 5.39. If (M^2 , g (t)) is a solution of the normalized Ricci
flow on a compact surf ace with R ( ·, 0) > 0, then
dN = - r iv R + R v f i 2 dA - 2 r i Ml2 dA :::; o,
dt }M2 R }M2
where M is the trace-free part of the Hessian off defined in (5.9). In
particular, the entropy is strictly decreasing unless (M^2 , g (t)) is a gradient
Ricci soliton.
PROOF. Recall that b..f = R - r. Expanding the first term on the
right-hand side and integrating by parts, we obtain
(5.26)
r IV' R + RV' fl
2
dA = r (IV' Rl
2
- 2R(R - r) + RIV f 1^2 ) dA.
}M2 R }M2 R
On the other hand, commuting covariant derivatives and integrating by parts
shows that
{ (R - r)^2 dA = { (b..f)^2 dA
}M2 }M2
hence that
= - f (Y' f, V' b..J) dA
}M2
= - { ( (V' f, b.. V' !) - Re (V' f, V' f)) dA
}M2
= JM 2 ( 1vv fl
2
+~R1v f l
2
) dA,
- 2 /M2 IMl2 dA = !M2 ( (b..f)2 - 2 IV'Y' f l2) dA
= JM2 (~RIV f l
2
- IVY' f l
2
) dA
(5.27) = JM 2 (RIV f l^2 - (R - r)^2 ) dA.
Subtracting (5.26) from (5.27) yields
- 2 r IMl2 dA - r IV' R +RV' f l2 dA = r ((R - r)2 - IV' Rl2) dA,
}M2 }M2 R }M2 R
whence the result follows by Lemma 5.38. D
COROLLARY 5.40. Let (M^2 , g (t)) be a solution of the normalized Ricci
flow on a closed surface with R (., 0) > 0. Then the entropy is a strictly-
decreasing function of time unless R (-, 0) = r, in which case it is constant
in time.