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Conformally Invariant Variational Problems. - SAM

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iemannian manifold (M m ,g). Let Ψ be a positive conformal<br />

diffeomorphism from (M m ,g) into another riemannian oriented<br />

manifold (N m ,k) then we have the following pointwise identity<br />

everywhere on Σ 2<br />

[<br />

| H ⃗ Φ ⃗ ∗g | 2 Φ<br />

−K ⃗ ∗g +K g] dvol ⃗Φ∗ g<br />

[<br />

= | H ⃗ (Ψ◦⃗ Φ) ∗k | 2 −K (Ψ◦⃗ Φ) ∗k +K k] dvol (Ψ◦Φ)∗ ⃗ k<br />

(X.47)<br />

where K g (resp. K k ) is the sectional curvature of the 2−plane<br />

⃗Φ ∗ TΣ 2 in (M m ,g) (resp. of the two plane Ψ ∗Φ∗ ⃗ TΣ 2 in (N m ,k)).<br />

In particular the following equality holds<br />

∫<br />

W( Φ)+ ⃗ K g dvol ⃗Φ∗ g<br />

Σ 2 ∫<br />

(X.48)<br />

= W(Ψ◦Φ)+<br />

⃗ K k dvol (Ψ◦Φ)∗ ⃗ g<br />

.<br />

Σ 2<br />

Proof of corollary X.1.<br />

By definition Ψ realizes an isometry between (M m ,Ψ ∗ k) and<br />

(N m ,k). Let µ ∈ R such that e µ g = Ψ ∗ k. We can apply the<br />

previous theorem with h = Ψ ∗ k and we obtain<br />

[<br />

| ⃗ H ⃗ Φ ∗g | 2 −K ⃗ Φ ∗ g<br />

]<br />

= e 2µ [<br />

| ⃗ H (Ψ◦⃗ Φ) ∗k | 2 −K (Ψ◦⃗ Φ) ∗ k<br />

]<br />

✷<br />

. (X.49)<br />

Itisalsoclearthatthevolumeformdvol g givenbytherestriction<br />

to Σ 2 of the metric g is equal to e −2µ dvol Ψ∗ k where dvol Ψ∗ k is<br />

equal to the volume form given by the restriction to Σ 2 of the<br />

metric Ψ ∗ k. Hence combining this last fact with (X.47). (X.48)<br />

is obtained by integrating (X.47) over Σ 2 , the scalar curvature<br />

terms canceling each other on both sides of the identity due to<br />

Gauss Bonnet theorem. Corollary X.1 is then proved. ✷<br />

120

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