- MONOTONICITY OF ENERGY FOR THE RICCI FLOW 201
sincefoT JM bOadμdt = foT JM b ( :t - ~) adμdt
= foT JM [a ( -:t - ~) bdμ - ab :t dμ] dt
= foT JM aO*bdμdt
for C^2 functions a and b on M x [O, T] with compact support in M x (0, T) ,where we used fft dμ = -Rdμ.
By (5.38), if (g (t), f (t)) is a solution to (5.34)-(5.35), then u = e-f
satisfies the adjoint heat equation (also known as the conjugate heat
equation)(5.40)It is often better to think in terms of u than in terms of f since u satisfies
the adjoint heat equation. In particular, the fundamental solution to the
adjoint heat equation is important.
2.3. Monotonicity of :F for the Ricci flow. In this subsection we
give two proofs of the monotonicity of energy for Ricci flow. In the next sec-
tion we give an application of this formula to the nonexistence of nontrivial
breather solutions.
2.3.1. Deriving the monotonicity of :F from the monotonicity of ;::m.
By the diffeomorphism invariance of all the quantities under consideration,
the monotonicity formula for the gradient flow implies a monotonicity
formula for the Ricci flow. This involves a function f (t) obtained by
solving the backward heat equation (5.35).
LEMMA 5.18 (:F energy monotonicity). If (g (t), f(t)) is a solution to
(5.34)-(5.35) on a closed manifold Mn, then(5.41) !:r:(g (t), f(t)) = 2 JM JRij + ViVjfl^2 e-f dμ.
PROOF. Since (g (t), f(t)) is a solution to (5.34)-(5.35), (g (t), J (t)),
defined by g(t) ~ <P*(t)g(t) and f(t) = f(t) o <P(t), where <P(t) satisfies
(5.36), is a solution to (5.29)-(5.30). Now :F (g, f) = :F (g, J) , so that by
(5.31), we havedt d :F (g ( t) ' f ( t)) = dt d :F ( g ( t) ' f -( t) )
= 2 JM \l~ij + ViVjfl~ e-f dP,
= 2 JM IRij + ViVjfl^2 e-f dμ.