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Conformally Invariant Variational Problems. - SAM

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where we used that the unit sphere is a constant sectional curvature<br />

space : for any two plane σ in TS m K Sm (σ) = 1. In<br />

the other hand the previous discussion leads to the following<br />

inequality<br />

∫<br />

liminf | H<br />

λ→+∞<br />

∫Σ ⃗ Ψλ ◦Φ ⃗|2 dvol (Ψλ ◦Φ) ⃗ ∗ g + S<br />

dvol 2 m (Ψλ ◦Φ) ⃗ ∗ g S<br />

Σ 2 m<br />

k∑<br />

∫<br />

≥ | H| ⃗ 2 g Sj<br />

dvol gSj +Area(S j ) .<br />

j=1 S j<br />

(X.61)<br />

For each S j there is an isometry of S m sending S j to the canonical<br />

2-sphere S 2 ⊂ R 3 ⊂ R m . S 2 is minimal in S m ( H ⃗ ≡ 0 ) and<br />

Area(S 2 ) = 4π. Thus we deduce that<br />

∫<br />

∀j = 1···k | H| ⃗ 2 g Sj<br />

dvol gSj +Area(S j ) = 4π . (X.62)<br />

S j<br />

Combining (X.60), (X.61) and (X.62) gives Li-Yau inequality<br />

(X.59).<br />

✷<br />

Li and Yau established moreover a connection between the<br />

Willmore energy of an immersed surface and it’s the conformal<br />

class that provided new lower bounds.<br />

Let Φ ⃗ be a conformal parametrization of the immersion of a<br />

riemann surface 44 (Σ 2 ,c) into S m . The m−conformal volume<br />

of Φ ⃗ is the following quantity<br />

∫<br />

V c (m, Φ) ⃗ = sup dvol ⃗Φ∗ Ψ ∗ g<br />

Ψ∈Conf(S m S<br />

.<br />

) Σ 2 m<br />

whereConf(S m )denotesthespaceofconformaldiffeomorphism<br />

of S m . Then Li and Yau define the m−conformal volume of a<br />

Rieman surface (Σ 2 ,c) to be the following quantity<br />

V c (m,(Σ 2 ,c)) = inf<br />

⃗Φ<br />

V c (m, ⃗ Φ)<br />

44 The pair (Σ 2 ,c) denotes a closed 2-dimensional manifold Σ 2 together with a fixed<br />

conformal class on this surface.<br />

127

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