Gibbons-type conjecture for abelian Higgs critical points

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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

lim⁡R→∞1∣BRn−2∣∫BRneε(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×Rn−2x=(y,z)\in\mathbb{R}^2\times\mathbb{R}^{n-2} and also assume

lim⁡∣y∣→∞∣u(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 Rn→R2\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.

References

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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