Conformally Invariant Variational Problems. - SAM
Conformally Invariant Variational Problems. - SAM
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