Extinction behaviour for the fast diffusion equations with critical exponent and Dirichlet boundary conditions

preprint2020arXivOpen access

Abstract

For a smooth bounded domain Ω⊆RnΩ\subseteq\mathbb{R}^n, n≥3n\geq 3, we consider the fast diffusion equation with critical sobolev exponent ∂w∂τ=Δwn−2n+2\frac{\partial w}{\partialτ} =Δw^{\frac{n-2}{n+2}} under Dirichlet boundary condition w(⋅,τ)=0w(\cdot, τ) = 0 on ∂Ω\partialΩ. Using the parabolic gluing method, we prove existence of an initial data w0w_0 such that the corresponding solution has extinction rate of the form ∥w(⋅,τ)∥L∞(Ω)=γ0(T−τ)n+24∣ln⁡(T−τ)∣n+22(n−2)(1+o(1))\|w(\cdot, τ)\|_{L^\infty(Ω)} = γ_0(T-τ)^{\frac{n+2}{4}}\left|\ln(T-τ)\right|^{\frac{n+2}{2(n-2)}}(1+o(1)) as t→T−t\to T^-, here T>0T > 0 is the finite extinction time of w(x,τ)w(x, τ). This generalizes and provides rigorous proof of a result of Galaktionov and King \cite{galaktionov2001fast} for the radially symmetric case Ω=B1(0):={x∈Rn∣∣x∣<1}⊂RnΩ=B_1(0) : = \{x\in \mathbb{R}^n||x| < 1\}\subset\mathbb{R}^n.

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