2018
DOI: 10.1093/imrn/rny012
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On Strongly Anisotropic Type I Blowup

Abstract: We consider the energy super critical 4 dimensional semilinear heat equation ∂tu = ∆u + |u| p−1 u, x ∈ R 4 , p > 5. Let Φ(r) be a three dimensional radial self similar solution for the three supercritical probmem as exhibited and studied in [7]. We show the finite codimensional transversal stability of the corresponding blow up solution by exhibiting a manifold of finite energy blow up solutions of the four dimensional problem with cylindrical symmetry which blows up asOur analysis revisits the stability analy… Show more

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Cited by 20 publications
(16 citation statements)
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“…In the supercritical and critical range in the Sobolev sense, type I blow-up is also known to occur for some solutions which are neither radial nor increasing in time: see [10] for N = 3, p > p S , [38] for N = 4, p > 5, [7] for N ≥ 7 and p = p S and [8] for p = p S . (ii) Type II blow-up.…”
Section: Resultsmentioning
confidence: 99%
“…In the supercritical and critical range in the Sobolev sense, type I blow-up is also known to occur for some solutions which are neither radial nor increasing in time: see [10] for N = 3, p > p S , [38] for N = 4, p > 5, [7] for N ≥ 7 and p = p S and [8] for p = p S . (ii) Type II blow-up.…”
Section: Resultsmentioning
confidence: 99%
“…Structure of the reconnection profile. In the companion paper [28], we address a similar result in the context of type I blow up with decreasing at infinity self similar profile. The analysis of type I blow up is simpler, and the reconnection profile is universal 14) which is reminiscent to the stability of the ODE type I blow up [2,29].…”
mentioning
confidence: 83%
“…Local asymptotic stability in the interior of the backward light (acoustic) cone from the singularity relies on an abstract spectral argument for compact perturbations of maximal accretive operators. Related arguments have been used in the literature for the study of self-similar solutions both in focusing and defocusing regimes, for example [8,16,21,45,47] for parabolic and [19] for hyperbolic problems. The key to the control of the nonlinear flow in the exterior of the light cone is the propagation of certain weighted scale invariant norms.…”
Section: Restriction On the Parametersmentioning
confidence: 99%