2012
DOI: 10.1007/s00526-012-0580-6
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Sharp energy estimates for nonlinear fractional diffusion equations

Abstract: Abstract. We study the nonlinear fractional equation (−∆) s u = f (u) in R n , for all fractions 0 < s < 1 and all nonlinearities f . For every fractional power s ∈ (0, 1), we obtain sharp energy estimates for bounded global minimizers and for bounded monotone solutions. They are sharp since they are optimal for solutions depending only on one Euclidian variable. As a consequence, we deduce the one-dimensional symmetry of bounded global minimizers and of bounded monotone solutions in dimension n = 3 whenever… Show more

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Cited by 79 publications
(94 citation statements)
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“…On the other hand, energy estimates for minimizers of non-local energies have been independently obtained in [CC14] and [SV14] (in different settings). Since both these two results were set in a slightly different framework than ours, we provide their proofs in full details in Sections 2 and 3, respectively.…”
Section: And (W4)mentioning
confidence: 99%
See 1 more Smart Citation
“…On the other hand, energy estimates for minimizers of non-local energies have been independently obtained in [CC14] and [SV14] (in different settings). Since both these two results were set in a slightly different framework than ours, we provide their proofs in full details in Sections 2 and 3, respectively.…”
Section: And (W4)mentioning
confidence: 99%
“…Estimate (3.2) has first been proved in [CC14] and [SV14] for the fractional Laplacian. While in the first paper the authors use the harmonic extension of u to R n+1 + to prove (3.2), in the latter work the result is obtained by explicitly computing the (5) We observe that, at this level, only the boundedness of W encoded in (W3) is relevant here.…”
Section: An Energy Estimatementioning
confidence: 99%
“…For the fractional case, the analogue of this 1 − D symmetry result for stable solutions of the equation (−Δu) s = f (u) has been proven to be true in dimension 2 for any power 0 < s < 1 [4,23] and in dimension 3 for 1/2 ≤ s < 1 [2,3]. The proofs of all these results make use of the extension established in [5], which allows to study the fractional equation (1.1) by studying a local Neumann problem in the half-space R n+1 + .…”
Section: Theorem 12mentioning
confidence: 99%
“…The proofs of all these results make use of the extension established in [5], which allows to study the fractional equation (1.1) by studying a local Neumann problem in the half-space R n+1 + . In [23], the authors used a geometric inequality analogue to (1.11) for the extended problem in the half-space, while in [2][3][4] a different approach based on a Liouville type result is used.…”
Section: Theorem 12mentioning
confidence: 99%
“…We will find a solution to (1) if we may construct a solution to (3). Denote w the unique solution of (−∂ xx ) s w − F (w(x)) = 0, w(0) = 0, w(±∞) = ±1.…”
Section: Introductionmentioning
confidence: 99%