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Conformally Invariant Variational Problems. - SAM

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defined by<br />

⎛<br />

Ω =<br />

⎜<br />

⎝<br />

0 −∇ ⊥ φ 0 −∇φ<br />

∇ ⊥ φ 0 ∇φ 0<br />

0 ∇φ 0 −∇ ⊥ φ<br />

−∇φ 0 ∇ ⊥ φ 0<br />

⎞<br />

⎟<br />

⎠<br />

(VII.37)<br />

Since φ ∈ W 2,1 , the following theorem VII.4 implies that<br />

∇W, and hence ∇u, belong to L p for some p > 2, thereby enabling<br />

the initialization of a bootstrapping argument analogous<br />

to that previously encountered in our study of the CMC equation.<br />

This procedure yields that u lies in W 2,q for all q < +∞.<br />

Owing to the standard Sobolev embedding theorem, it follows<br />

that u ∈ C 1,α , which concludes the proof of the desired theorem<br />

VII.2 in the case when the target manifold of the harmonic<br />

map u is the two-torus.<br />

✷<br />

Theorem VII.4. Let W be a solution in W 1,2 (D 2 ,R n ) of the<br />

linear system<br />

−∆W = Ω·∇W , (VII.38)<br />

where Ω is a W 1,1 vector field on D 2 taking values in the space<br />

of n×n matrices. Then W belongs to W 1,p (B 1/2 (0)), for some<br />

p > 2. In particular, W is Hölder continuous 18 19 . ✷<br />

Proof of theorem VII.4.<br />

18 The statement of theorem VII.4 is optimal. To see this, consider u = loglog1/r = W.<br />

One verifies easily that u ∈ W 1,2 (D 2 ,T 2 ) satisfies weakly (VI.26). Yet, Ω ≡ ∇u fails to<br />

be W 1,1 , owing to<br />

∫ 1<br />

dr<br />

0 rlog 1 = +∞ .<br />

r<br />

19 The hypothesis Ω ∈ W 1,1 may be replaced by the condition that Ω ∈ L 2,1 .<br />

72

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