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Conformally Invariant Variational Problems. - SAM

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following equation<br />

⎧ [ ]<br />

∂ ⎪⎨<br />

ij ∂λ<br />

a = ∂a ∂b<br />

− ∂a ∂b<br />

on D 2<br />

∂x i ∂x j ∂x 1 ∂x 2 ∂x 2 ∂x 1<br />

⎪⎩<br />

ϕ = 0 on ∂D 2 .<br />

(X.161)<br />

Then ϕ ∈ L ∞ ∩W 1,2 (D 2 ,R) and there exists C > 0 independent<br />

of a and b such that<br />

‖ϕ‖ L<br />

∞ +‖∇ϕ‖ L<br />

2 ≤ C ‖∇a‖ L<br />

2 ‖∇b‖ L<br />

2 . (X.162)<br />

Using theorem X.11 we obtain that λ ∈ L ∞ (D 2 ,R). Let e i<br />

be the frame on D 2 given by<br />

✷<br />

d ⃗ Φ·e i =⃗e i<br />

and denote e i = e 1 i ∂ x 1<br />

+e 2 i ∂ x 2<br />

. We have<br />

2∑<br />

e k i g kj = .<br />

k=1<br />

from which we deduce<br />

2∑<br />

e k i = g kj <br />

j=1<br />

Because of (X.145) the maps g kj are in L ∞ . Thus<br />

2∑ [<br />

e ∗ i = g 1j dx1<br />

j=1<br />

+g 2j dx2<br />

]<br />

∈ L ∞ (D 2 ) .<br />

(X.163)<br />

Denote by (f 1 ,f 2 ) the frame on D 2 such that d ⃗ Φ · f i = ⃗ f i , we<br />

have f a st = f ∗ 1 + if∗ 2 = e−iθ (e ∗ 1 + ie∗ 2 ) which is in L∞ (D 2 ) due<br />

to (X.163). Hence the map φ = (φ 1 ,φ 2 ) which is given by<br />

dφ i := e −λ f ∗ i .<br />

172

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