2019
DOI: 10.2140/tunis.2019.1.13
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Construction of a stable blowup solution with a prescribed behavior for a non-scaling-invariant semilinear heat equation

Abstract: We consider the semilinear heat equationin the whole space ‫ޒ‬ n , where p > 1 and α ∈ ‫.ޒ‬ Unlike the standard case α = 0, this equation is not scaling invariant. We construct for this equation a solution which blows up in finite time T only at one blowup point a, according to the asymptotic dynamicwhere ψ(t) is the unique positive solution of the ODEThe construction relies on the reduction of the problem to a finite-dimensional one and a topological argument based on the index theory to get the conclusion. B… Show more

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Cited by 27 publications
(31 citation statements)
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“…(1. 4) In addition to that, in [13], Herrero and Velázquez derived the same result with a different method. Particularly, in [17], Merle and Zaag gave a proof which is simpler than the one in [1] and proposed the following two-step method (see also the note [15]):…”
Section: Ealier Workmentioning
confidence: 62%
See 1 more Smart Citation
“…(1. 4) In addition to that, in [13], Herrero and Velázquez derived the same result with a different method. Particularly, in [17], Merle and Zaag gave a proof which is simpler than the one in [1] and proposed the following two-step method (see also the note [15]):…”
Section: Ealier Workmentioning
confidence: 62%
“…and also the work of Duong, Nguyen and Zaag in [4], who considered the following non scale invariant equation ∂ t u = ∆u + |u| p−1 u ln α (2 + u 2 ).…”
Section: Ealier Workmentioning
confidence: 99%
“…Let us mention that the blow-up question for the semilinear heat equation ∂ t u = ∆u + |u| p−1 u log a (2 + u 2 ) is studied by Duong-Nguyen-Zaag in [18]. More precisely, they construct for this equation a solution which blows up in finite time T , only at one blow-up point a, according to the following asymptotic dynamics:…”
Section: Introductionmentioning
confidence: 99%
“…This two-step procedure has been successfully applied for various nonlinear evolution equations to construct both Type I and Type II blowup solutions. It was the case of the semilinear heat equation treated in [4], [32], [36] (see also [35], [9] for the case of logarithmic perturbations, [2], [3] and [16] for the exponential source, [37] for the complex-valued case), the Ginzburg-Landau equation in [27], [38] (see also [48] for an earlier work). It was also the nonlinear Schrödinger equation both in the mass critical [28,29,30,31] and mass supercritical [34] cases; the energy critical [10], [22] and supercritical [6] wave equation; the mass critical gKdV equation [24,25,26]; the two dimensional Keller-Segel model [42]; the energy critical and supercritical geometric equations: the wave maps [39] and [18], the Schrödinger maps [33] and the harmonic heat flow [40,41] and [17]; the semilinear heat equation in the energy critical [43] and supercritical [5] cases.…”
Section: Introductionmentioning
confidence: 99%