三维能量临界热方程的无限时间爆破
偏微分方程分析
2020-01-08 v4
摘要
我们构造了三维能量临界热方程在时间上全局定义、无界正解 u t = Δ u + u 5 , \mbox i n R 3 × ( 0 , ∞ ) , u ( x , 0 ) = u 0 ( x ) \inn R 3 . u_t = \Delta u + u^5 , \quad {\mbox {in}} \quad \R^3 \times (0,\infty), \ \ u(x, 0)= u_0 (x)\inn \R^3. u t = Δ u + u 5 , \mbox in R 3 × ( 0 , ∞ ) , u ( x , 0 ) = u 0 ( x ) \inn R 3 . 对于每个γ > 1 \gamma>1 γ > 1 ,我们找到初始数据(不一定径向对称)满足lim r → ∞ ∣ x ∣ γ u 0 ( x ) > 0 \lim\limits_{r \to \infty} |x|^\gamma u_0 (x) >0 r → ∞ lim ∣ x ∣ γ u 0 ( x ) > 0 ,使得当t → ∞ t \to \infty t → ∞ 时 ∥ u ( ⋅ , t ) ∥ ∞ ∼ t γ − 1 2 , \mbox i f 1 < γ < 2 , ∥ u ( ⋅ , t ) ∥ ∞ ∼ t , \mbox i f γ > 2 , \| u(\cdot ,t ) \|_\infty \sim t^{\gamma-1 \over 2} , \quad {\mbox {if}} \quad 1<\gamma <2, \quad \| u(\cdot ,t ) \|_\infty \sim \sqrt{t}, \quad {\mbox {if}} \quad \gamma >2, \quad ∥ u ( ⋅ , t ) ∥ ∞ ∼ t 2 γ − 1 , \mbox i f 1 < γ < 2 , ∥ u ( ⋅ , t ) ∥ ∞ ∼ t , \mbox i f γ > 2 , 且 ∥ u ( ⋅ , t ) ∥ ∞ ∼ t ( ln t ) − 1 , \mbox i f γ = 2. \| u(\cdot , t)\|_\infty \sim \sqrt{t}\, (\ln t )^{-1} , \quad {\mbox {if}} \quad \gamma = 2. ∥ u ( ⋅ , t ) ∥ ∞ ∼ t ( ln t ) − 1 , \mbox i f γ = 2. 此外我们证明这种无限时间爆破是余维一稳定的。Fila和King曾猜想此类解的存在。
引用
@article{arxiv.1705.01672,
title = {Infinite time blow-up for the 3-dimensional energy critical heat equation},
author = {Manuel del Pino and Monica Musso and Juncheng Wei},
journal= {arXiv preprint arXiv:1705.01672},
year = {2020}
}