Sharp Transition Between Extinction and Propagation of Reaction
Andrej Zlatos
TL;DR
The paper analyzes extinction versus propagation for the 1D reaction-diffusion equation $T_t = T_{xx} + f(T)$ with compactly supported initial data, covering ignition, combustion, and bistable nonlinearities. It develops a scaling- and comparison-based framework to identify a unique critical length $L_0$ separating quenching from propagation, establishing that $L_0 = L_1$ in the ignition setting. At criticality, the long-time limit at the origin is a fixed point of $f$ (for ignition) or a nontrivial stationary bell-shaped profile $U$ solving $0=U''+f(U)$ (for bistable/combustion), yielding a complete phase portrait for the 1-parameter initial data family. The results extend classical Kanel’ theory, show robustness to advection, and provide a unified approach to extinction thresholds across nonlinearities.
Abstract
We consider the reaction-diffusion equation \[ T_t = T_{xx} + f(T) \] on $\bbR$ with $T_0(x) \equiv \chi_{[-L,L]} (x)$ and $f(0)=f(1)=0$. In 1964 Kanel' proved that if $f$ is an ignition non-linearity, then $T\to 0$ as $t\to\infty$ when $L<L_0$, and $T\to 1$ when $L>L_1$. We answer the open question of relation of $L_0$ and $L_1$ by showing that $L_0=L_1$. We also determine the large time limit of $T$ in the critical case $L=L_0$, thus providing the phase portrait for the above PDE with respect to a 1-parameter family of initial data. Analogous results for combustion and bistable non-linearities are proved as well.
