2017
DOI: 10.1007/s00526-017-1256-z
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Stable self-similar blowup in the supercritical heat flow of harmonic maps

Abstract: We consider the heat flow of corotational harmonic maps from R 3 to the threesphere and prove the nonlinear asymptotic stability of a particular self-similar shrinker that is not known in closed form. Our method provides a novel, systematic, robust, and constructive approach to the stability analysis of self-similar blowup in parabolic evolution equations. In particular, we completely avoid using delicate Lyapunov functionals, monotonicity formulas, indirect arguments, or fragile parabolic structure like the m… Show more

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Cited by 8 publications
(9 citation statements)
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“…where Q corresponds to the unique (up to scaling) harmonic map in this class, and L ∈ Z + , with L = 1 providing the generic blow-up rate. See also [14] for a related recent result, and [5,6,20,21] concerning the breakdown of solutions in higher (supercritical) dimensions.…”
Section: Introduction and Resultsmentioning
confidence: 99%
“…where Q corresponds to the unique (up to scaling) harmonic map in this class, and L ∈ Z + , with L = 1 providing the generic blow-up rate. See also [14] for a related recent result, and [5,6,20,21] concerning the breakdown of solutions in higher (supercritical) dimensions.…”
Section: Introduction and Resultsmentioning
confidence: 99%
“…Our estimates (1.3) on f 0 lead to very precise bounds on V 0 and in turn allow us to prove the following stability result. This result is an indispensable ingredient in the proof of the nonlinear asymptotic stability of f 0 in the companion paper [4].…”
Section: Introductionmentioning
confidence: 90%
“…In addition to the existence result we have the following technical proposition to describe some qualitative properties of f 0 needed in the proof of nonlinear stability in [4].…”
Section: Introductionmentioning
confidence: 99%
“…The harmonic map heat flow forms also singularity in finite time, and the self-similar nature of the singularity appears only when 3 ≤ d ≤ 6, and for d ≥ 7 self-similar blowup solutions don't exist [6]. For 3 ≤ d ≤ 6, the existence of the self-similar solutions is known [13] and the stability has been proved only in the case d = 3 as in [1]. When d = 7 the blowup is not self-similar and the speed λ has a log correction [15], it turns out that the non-self-similar regime is stable when d = 7.…”
Section: Introductionmentioning
confidence: 99%