2013
DOI: 10.1515/acv-2012-0104
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Estimates for the energy density of critical points of a class of conformally invariant variational problems

Abstract: Abstract. We show that the energy density of critical points of a class of conformally invariant variational problems with small energy on the unit 2-disk B 1 ⊂ R 2 lies in the local Hardy space h 1 (B 1 ). As a corollary we obtain a new proof of the energy convexity and uniqueness result for weakly harmonic maps with small energy on B 1 .

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Cited by 16 publications
(26 citation statements)
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“…Now using (18) and by the results of Coifman-Lions-Meyer-Semmes [5] or Wente's lemma [53], we know (25) B L ∞ (Dr(p)) + ∇B L 2,1 (Dr(p)) ≤ C ∇ũ 2 L 2 (Dr(p)) . Therefore, combining (16), (22), (24) and (25) we have…”
Section: Lemma 24 (Hardy's Inequalitymentioning
confidence: 99%
“…Now using (18) and by the results of Coifman-Lions-Meyer-Semmes [5] or Wente's lemma [53], we know (25) B L ∞ (Dr(p)) + ∇B L 2,1 (Dr(p)) ≤ C ∇ũ 2 L 2 (Dr(p)) . Therefore, combining (16), (22), (24) and (25) we have…”
Section: Lemma 24 (Hardy's Inequalitymentioning
confidence: 99%
“…Now we check how P transforms ω, by (7) we have P −1 dP + P −1 ωP = ω P = d * η + P −1 d * bP ∈ L (2,1) (D) (8) and…”
Section: Proof Of the Regularity Result Corollary 22mentioning
confidence: 99%
“…In section 3 we show that critical points of conformally invariant elliptic Lagrangians solve (2) and, under an added regularity assumption, we can find the frame S solving (1). Unlike the case for harmonic maps we require the theory of Rivière, namely the existence of the frame A solving (4), in order to find S. However this can still be used to re-prove a recent estimate of Lamm and Lin [8], Theorem 3.3. We remark that it might be possible to drop the added regularity and still be able to find S in this setting; either a positive or a negative answer to this question would provide further insight into these regularity problems.…”
Section: Introductionmentioning
confidence: 99%
“…Besides the uniqueness consequence, this theorem is very useful for many other problems such as flow convergence, see [25]. In fact our proof simplifies the original proof by Colding-Minicozzi and the one of Lamm-Lin [22]. In fact our idea applies probably to all conformally invariant problem, since it relies only on the ε-regularity, the fact that the right hand side of the equation is orthogonal to T N .…”
Section: Step 2: Convexity For Free Boundary Energymentioning
confidence: 90%