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Conformally Invariant Variational Problems. - SAM

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either ∂ z u = 1 2 (∂ x 1<br />

u−i∂ x2 u) ≡ 0<br />

(II.7)<br />

or ∂¯z u = 1 2 (∂ x 1<br />

u+i x2 u) ≡ 0<br />

(II.8)<br />

✷<br />

Proof of Proposition II.1<br />

Because of (II.1) a map u from a 2-dimensional domain U of<br />

C into a manifold (N n ,h) is conformal if and only if one has<br />

⎧<br />

⎨ < ∂ x1 u,∂ x2 u > h = 0<br />

(II.9)<br />

⎩<br />

| ∂ x1 u | h =| ∂ x2 u | h<br />

in the case of U : U CC −→ C a direct computation gives<br />

∂u<br />

∂z<br />

∂ū<br />

∂z = 1 4 [(∂ x 1<br />

u 1 +∂ x2 u 2 )+i(∂ x1 u 2 −∂ x2 u 1 )]<br />

[(∂ x1 u 1 −∂ x2 u 2 )−i(∂ x2 u 1 +∂ x1 u 2 )]<br />

(II.10)<br />

= 1 4<br />

[<br />

| ∂x1 u | 2 − | ∂ x2 u | 2 −2i < ∂ x1 u,∂ x2 u > ]<br />

where < ·,· > denotes the scalar product in C. Observe that<br />

the quadratic 1−0⊗1−0 form Φ(u) given by<br />

Φ(u) = ∂u<br />

∂z<br />

∂ū<br />

∂z<br />

dz ⊗dz<br />

is invariant under holomorphic change of coordinates:<br />

for w(z) satisfying ∂¯z w = 0 one has locally away from zeros<br />

of w ′<br />

φ(u) = ∂u<br />

∂w<br />

∂ū<br />

∂w dw⊗dw<br />

6

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