Extinction rates for nonradial solutions to the Stefan problem
Gabriele Fioravanti, Xavier Ros-Oton, Clara Torres-Latorre
TL;DR
This work analyzes the one-phase Stefan problem and its free boundary near isolated singular points. By employing second-blow-up analysis, expansion at singular points, and parabolic barrier constructions, the authors derive sharp melting-rate bounds in 2D that closely mirror radial solutions and extend to higher dimensions with precise, stratified behavior. They establish global C^1 regularity of the free boundary away from the top stratum Σ_{n-1}, and show that Γ(x) = t is not C^1 on Σ_{n-1}, with optimal notations tied to extinction rates. The results provide a deep, quantitative description of the free boundary structure, including a thorough treatment of singular sets via self-similar caloric solutions and Whitney-type regularity, significantly advancing the understanding of the Stefan problem’s singularities and regularity theory.
Abstract
We consider the one-phase Stefan problem describing the evolution of melting ice. On the one hand, we focus on understanding the evolution of the free boundary near isolated singular points, and we establish for the first time upper and (more surprisingly) lower estimates for its evolution. In 2D, these bounds almost match the best known ones for radial solutions, but hold for all solutions to the Stefan problem, with no extra assumption on the initial or boundary data. On the other hand, as a consequence of our results, we also characterize the global regularity of the free boundary, as follows: it can be written as a graph $t = Γ(x)$, where $Γ$ is $C^1$ (and not $C^2$) near any singular points in the lower strata $Σ_m$, $m \leq n - 2$. Moreover, $Γ$ is not $C^1$ at singular points in $Σ_{n-1}$.
