- HARMONIC MAPS PARAMETRIZING ALMOST HYPERBOLIC PIECES 221
Since <Pi gi converges to hl1-l A/2 in C^00 , we have that
i-+cx::> lim u T;~-+ l fJHA,
EE£(K)
where this convergence is also inc= (compare with (34.70) in the next chapter).
Hence there exist diffeomorphisms
Wi: (HA, hj1-lJ-+ (Hi,A, <P;gi)
which are close to isometries in the sense that for all k E NU {O} ,^4
(33.5)
Since 8Hi,A is CMC with respect to <P; g;, we have that &HA is also CMC with
respect to Wi<Pigi.
Since &HA is totally umbillic and strictly concave in (HA, hl1-lJ, by (33.5) and
Proposition 33.12, for i sufficiently large there exists a unique harmonic diffeomor-
phism
ci: (HA, hl1-lJ-+ (HA, w;<P;gi)
close to the identity map satisfying Ci(EJHA) = &HA and (Ci)* (N) is normal to
8HA with respect to Wi<Pi gi. Here N is the unit outward normal vector to &HA
with respect to h. We then have that
Fi~ <Pio Wi o Ci : (HA, hl1-lJ-+ (Mi, gi)
is a harmonic embedding satisfying the CMC boundary conditions. Note that
Fi (&HA)= (<Pio wi) (EJHA) = <Pi(Uea(JC) T;~).
By (33.5) and since the h armonic diffeomorphism Ci is obtained by the implicit
function theorem, we have for any k EN,
as i -+ oo. Finally, since <Pi (x 00 ) =Xi, we have that
as i -+ oo since wi and Ci both tend to the identity. This completes the proof of
Proposition 33.13. 0
2.2. Continuing harmonic parametrizations of almost hyperbolic
pieces.
The result of this subsection states that if we are given a family of metrics
g (t), t E [a, w], on a 3-manifold M^3 (such as a solution to the NRF) and an almost
isometric harmonic embedding Fa into ( M, g (a)) from a truncated hyperbolic 3-
manifold satisfying the CMC boundary conditions, then we may extend Fa to a
I-parameter family of almost isometric harmonic embeddings F ( t) into ( M, g ( t))
for t 2 a satisfying the CMC boundary conditions and defined so long as F (t)
remains sufficiently close to an isometry.
(^4) To accomplish this, we only need to perturb Wi away from the identity in a collar of 811.A
in 1iA· HINT: Write 811.;,A as a graph over 811.A·