4. RELATION TO THE HARMONIC MAP FLOW 85
Hence
\7 (df) = L (\7df)0 dxi 0 dxj 0
0
° a
i,J,a .. y
where
The harmonic map Laplacian with respect to the domain metric g
and codomain metric h is defined to be the trace
namely
.. a
~ g, hf= (gi^3 \7·d·f'Y) i J [)yr -.
In components,
Given Jo : Mn ---+ Nm, the harmonic map fl.ow introduced by Eells
and Sampson is
(3.40a)
(3.40b)
of_~
at - g,h^1 '
f (0) = fo.
This is a parabolic equation, so a unique solution exists for a short time.
When f is a diffeomorphism, the Laplacian ~g,hf may be rewritten in
a useful way:
LEMMA 3.18. Let f: (Mn,g)---+ (Nn,h) be a diffeomorphism of Rie-
mannian manifolds. Then
PROOF. We first compute the Christoffel symbols of the pull-back of a