Exterior-domain rigidity conjecture for the discrete-time overdetermined heat problem

Let N2N\ge 2 and let ΩRN\Omega\subset\mathbb{R}^N be an exterior domain, meaning the complement of a bounded closed set. Consider the initial-boundary value problem

{tu=Δuin Ω×(0,),u=1on Ω×{0},u=0on Ω×(0,),u(x,t)0uniformly in t as x.\begin{cases} \partial_t u=\Delta u & \text{in }\Omega\times(0,\infty),\\ u=1 & \text{on }\Omega\times\{0\},\\ u=0 & \text{on }\partial\Omega\times(0,\infty),\\ u(x,t)\to 0 & \text{uniformly in $t$ as $|x|\to\infty$}. \end{cases}

Exterior-domain rigidity conjecture. Complements of closed balls are the only exterior domains whose solution satisfies the discrete-time overdetermined boundary condition.

This is the unbounded-domain analogue of the rigidity problem for the overdetermined heat equation. The conjecture is motivated by continuous-time results obtained using moving planes, but the discrete-time condition and the lack of compactness in unbounded domains make the corresponding classification problem unresolved.

Sources & referencesView supporting material

Primary source

Lorenzo Cavallina and Andrea Pinamonti, “A discrete-time overdetermined problem for the heat equation”, arXiv:2604.20430 (2026).

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