Conformally Invariant Variational Problems. - SAM
Conformally Invariant Variational Problems. - SAM
Conformally Invariant Variational Problems. - SAM
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the whole regularity result stated in the theorem by using the<br />
following lemma.<br />
Lemma VIII.1. Let m ∈ N \ {0} and u ∈ W 1,p<br />
loc (D2 ,R m ) for<br />
some p > 2 satisfying<br />
−∆u = Ω·∇u<br />
where 24 Ω ∈ L 2 (D 2 ,M m (R) ⊗ R 2 ) then u ∈ W 1,q<br />
loc (D2 ,R m ) for<br />
any q < +∞.<br />
✷<br />
Let ε 0 > 0 be some constant whose value will be adjusted in<br />
due time to fit our needs. There exists a radius ρ 0 such that for<br />
every r < ρ 0 and every point p dans B 1/2 (0), there holds<br />
∫<br />
|∇A| 2 +|∇B| 2 < ε 0 . (VIII.15)<br />
B r (p)<br />
Henceforth, we consider only radii r < ρ 0 .<br />
Note that A∇u satisfies the elliptic system<br />
⎧<br />
⎨ div(A∇u) = ∇B ·∇ ⊥ u = ∂ y B∂ x u−∂ x B∂ y u<br />
⎩<br />
rot(A∇u) = −∇A·∇ ⊥ u = ∂ x A∂ y u−∂ y A∂ x u<br />
We proceed by introducing on B r (p) the linear Hodge decomposition<br />
in L 2 of A∇u. Namely, there exist two functions C and<br />
D, unique up toadditiveconstants, elementsof W 1,2<br />
0 (B r (p))and<br />
W 1,2 (B r (p)) respectively, and such that<br />
A∇u = ∇C +∇ ⊥ D .<br />
(VIII.16)<br />
To see why such C and D do indeed exist, consider first the<br />
equation<br />
⎧<br />
⎨ ∆C = div(A∇u) = ∂ y B∂ x u−∂ x B∂ y u<br />
(VIII.17)<br />
⎩<br />
C = 0 .<br />
24 Observe that in this lemma no antisymmetry assumption is made for Ω which is an<br />
arbitrary m×m−matrix valued L 2 −vectorfield on D 2 .<br />
83