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Conformally Invariant Variational Problems. - SAM

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First of all, it is clear that theorem VIII.1 is applicable to the<br />

equation (VIII.4) so as to yield the regularity of harmonic maps<br />

taking values in a manifold of codimension 1.<br />

Another rather direct application of theorem VIII.1 deals<br />

with the solutions of the prescribed mean curvature equation<br />

in R 3 ,<br />

∆u = 2H(u) ∂ x u×∂ y u dans D ′ (D 2 ) .<br />

This equation can be recast in the form<br />

∆u = H(u)∇ ⊥ u×∇u ,<br />

Via introducing<br />

⎛<br />

Ω := H(u) ⎜<br />

⎝<br />

0 −∇ ⊥ u 3 ∇ ⊥ u 2<br />

∇ ⊥ u 3 0 −∇ ⊥ u 1<br />

−∇ ⊥ u 2 ∇ ⊥ u 1 0<br />

⎞<br />

⎟<br />

⎠<br />

we observe successively that Ω is antisymmetric, that it belongs<br />

to L 2 whenever H belongs to L ∞ , and that u satisfies (VIII.6).<br />

The hypotheses of theorem VIII.1 are thus all satisfied, and so<br />

we conclude that that u is Hölder continuous.<br />

This last example outlines clearly the usefulness of theoremVIII.1towardssolvingHeinz-Hildebrandt’sconjecture.<br />

Namely,<br />

it enablesus to weakenthe Lipschitzeanassumptionon H found<br />

in previous works ([Hei1], [Hei2], [Gr2], [Bet1], ...), by only requiring<br />

that H be an element of L ∞ . This is precisely the condition<br />

stated in Hildebrandt’s conjecture. By all means, we are<br />

in good shape.<br />

In fact, Hildebrandt’s conjecture will be completely resolved<br />

with the help of the following result.<br />

78

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