Critical-parameter dichotomy conjecture for the nonlocal parabolic MEMS equation

Let ΩRN\Omega\subset\mathbb{R}^N, with 1N31\leq N\leq 3, be a bounded domain with smooth boundary, and let u0H2H01(Ω)u_0\in H^2\cap H_0^1(\Omega). Consider equation (1.1), its solution uλu_\lambda, and the steady-state equation (1.4). Critical-parameter dichotomy conjecture. There exists λ>0\lambda^{*}>0 such that, for λ<λ\lambda<\lambda^{*}, equation (1.1) has a unique global solution uλu_\lambda converging to a steady state as tt\to\infty, whereas, for λ>λ\lambda>\lambda^{*}, the solution quenches in finite time and equation (1.4) has no solution. This conjecture proposes a threshold separating global convergence from finite-time quenching and nonexistence of steady states, based on the paper's numerical experiments.

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Primary source

Yufei Wei and Yanyan Zhang, “Well-posedness and asymptotic behavior of solutions to a second order nonlocal parabolic MEMS equation”, arXiv:2603.07013 (2026).

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