English

A type II blowup for the six dimensional energy critical heat equation

Analysis of PDEs 2020-02-04 v1

Abstract

We study blowup solutions of the 6D energy critical heat equation ut=Δu+up1uu_t=\Delta u+|u|^{p-1}u in Rn×(0,T)\R^n\times(0,T). A goal of this paper is to show the existence of type II blowup solutions predicted by Filippas, Herrero and Vel\'azquez \cite{FilippasHV}. The dimension six is a border case whether a type II blowup can occur or not. Therefore the behavior of the solution is quite different from other cases. In fact, our solution behaves like u(x,t){λ(t)2Q(λ(t)1x)in the inner region: xλ(t),(p1)1p1(Tt)1p1in the selfsimilar region: xTt u(x,t)\approx \begin{cases} \lambda(t)^{-2}{\sf Q}(\lambda(t)^{-1}x) & \text{in the inner region: } |x|\sim\lambda(t), -(p-1)^\frac{1}{p-1}(T-t)^{-\frac{1}{p-1}} & \text{in the selfsimilar region: } |x|\sim\sqrt{T-t} \end{cases} with λ(t)=(1+o(1))(Tt)54log(Tt)158\lambda(t)=(1+o(1))(T-t)^\frac{5}{4}|\log(T-t)|^{-\frac{15}{8}}. The local energy Eloc(u)=12uL2(x<1)213uL3(x<1)3E_\text{loc}(u) =\frac{1}{2}\|\nabla u\|_{L^2(|x|<1)}^2-\frac{1}{3}\|u\|_{L^3(|x|<1)}^3 of the solution goes to -\infty.

Keywords

Cite

@article{arxiv.2002.00528,
  title  = {A type II blowup for the six dimensional energy critical heat equation},
  author = {Junichi Harada},
  journal= {arXiv preprint arXiv:2002.00528},
  year   = {2020}
}