Shnirelman–Šverák relaxation conjecture for two-dimensional Euler flows

Let ΩR2\Omega\subset\mathbb{R}^2 be a smooth bounded domain, let St:L(Ω)L(Ω)S_t:L^\infty(\Omega)\to L^\infty(\Omega) denote the two-dimensional Euler solution operator acting on vorticity, and define the weak limit set

A:={fL(Ω):Stn(ω0)f for some ω0L(Ω) and tn}.\mathcal{A}_\infty:=\left\{f\in L^\infty(\Omega): S_{t_n}(\omega_0)\rightharpoonup f\text{ for some }\omega_0\in L^\infty(\Omega)\text{ and }t_n\to\infty\right\}.

Shnirelman–Šverák relaxation conjecture. The set A\mathcal{A}_\infty consists of precisely those fL(Ω)f\in L^\infty(\Omega) for which {St(f)}tR\{\mathcal{S}_t(f)\}_{t\in\mathbb{R}} is pre-compact in L2(Ω)L^2(\Omega); moreover, for generic fL(Ω)f\in L^\infty(\Omega), the orbit {St(f)}tR\{S_t(f)\}_{t\in\mathbb{R}} is not pre-compact in L2(Ω)L^2(\Omega). This conjecture describes the expected long-time simplification of bounded-vorticity solutions of the two-dimensional Euler equation, distinguishing data with pre-compact dynamics from generic data whose trajectories fail to be pre-compact. The source attributes it to Shnirelman and Šverák; no resolution is supplied here.

Sources & referencesView supporting material

Primary source

Tarek M. Elgindi, “Dynamics of Ideal Fluid Flows”, arXiv:2511.16254 (2025).

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