Gibbons-type conjecture for abelian Higgs critical points

Let (u,)(u,\nabla) be an entire critical point on Rn\mathbb{R}^n, and let eε(u,)e_\varepsilon(u,\nabla) denote its energy density. Assume

limR1BRn2BRneε(u,)=2π.\lim_{R\to\infty}\frac{1}{|B_R^{n-2}|}\int_{B_R^n}e_\varepsilon(u,\nabla)=2\pi.

Write x=(y,z)R2×Rn2x=(y,z)\in\mathbb{R}^2\times\mathbb{R}^{n-2} and also assume

limyu(y,z)=1,uniformly in z.\lim_{|y|\to\infty}|u(y,z)|=1, \quad\text{uniformly in }z.

Gibbons-type conjecture. The critical point is necessarily two-dimensional: it is the pullback under the projection RnR2\mathbb{R}^n\to\mathbb{R}^2 of the standard degree ±1\pm1 solution in R2\mathbb{R}^2, up to translation and gauge change. The excerpt presents this as a variant of the Gibbons conjecture and says that the available techniques do not currently establish the conclusion.

Sources & referencesView supporting material

Primary source

Guido De Philippis, Aria Halavati and Alessandro Pigati, “Decay of excess for the abelian Higgs model”, arXiv:2405.13953 (2024).

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