Sharp threshold for a one-dimensional thin film equation in the supercritical case
Shen Bian

TL;DR
This paper analyzes a one-dimensional thin film equation with aggregation and repulsion, establishing a sharp threshold based on the steady state to predict finite-time blow-up or global existence of solutions.
Contribution
It introduces a variational characterization of the steady state and derives a precise criterion for blow-up versus global existence based on initial data norms.
Findings
Existence and uniqueness of a steady state $U_*$ for all $m>0$
Finite-time blow-up occurs if initial free energy is below $F(U_*)$ and $L^{m+1}$-norm exceeds that of $U_*$.
Solutions exist globally if the $L^{m+1}$-norm is below that of $U_*$, with divergence of second moment as $t oinity$.
Abstract
We study a one-dimensional thin film equation combining competitive effects of aggregation and repulsion, where repulsion is modeled by fourth-order diffusion and aggregation by backward second-order degenerate diffusion with exponent . Under natural regularity constraints, we prove that for every , there exists a unique (up to the mass-critical case ) nonnegative, radially decreasing steady state which coincides with the extremal function of the sharp Sz.-Nagy inequality and is simultaneously the global minimizer of the free energy. Using this variational characterization in the supercritical regime , we show that finite-time blow-up occurs for all initial data whose initial free energy lies below the positive threshold , provided the -norm of the initial datum exceeds that of . Conversely, if the -norm is below that of…
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