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De Giorgi's conjecture on monotone solutions of the Allen-Cahn equation

Theorem 1.1: every u∈C2(R8,(−1,1))u\in C^2(\mathbb R^8,(-1,1)) with Δu=u3−u\Delta u=u^3-u and ∂8u>0\partial_8u>0 equals tanh⁡((e⋅x−c)/2)\tanh((e\cdot x-c)/\sqrt2) with e8>0e_8>0. Theorem 1.2: every stable solution v:R7→[−1,1]v:\mathbb R^7\to[-1,1] is ±1\pm1 or planar, without an energy-growth assumption; this is sharp by Pacard-Wei's nonplanar stable solutions in R8\mathbb R^8. A final section explains why the argument fails in dimension nine, consistent with del Pino-Kowalczyk-Wei. The paper does not treat other potentials, the stable De Giorgi problem in dimension eight, or the Gibbons and Savin variants beyond what the monotone theorem implies.

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Occurred: Sep 26, 2026

Delta type: SOURCE CLAIM

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Canonical aliases: De Giorgi's conjecture on monotone solutions of the Allen-Cahn equation · De Giorgi's conjecture

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Theorem 1.1: every u∈C2(R8,(−1,1))u\in C^2(\mathbb R^8,(-1,1)) with Δu=u3−u\Delta u=u^3-u and ∂8u>0\partial_8u>0 equals tanh⁡((e⋅x−c)/2)\tanh((e\cdot x-c)/\sqrt2) with e8>0e_8>0. Theorem 1.2: every stable solution v:R7→[−1,1]v:\mathbb R^7\to[-1,1] is ±1\pm1 or planar, without an energy-growth assumption; this is sharp by Pacard-Wei's nonplanar stable solutions in R8\mathbb R^8. A final section explains why the argument fails in dimension nine, consistent with del Pino-Kowalczyk-Wei. The paper does not treat other potentials, the stable De Giorgi problem in dimension eight, or the Gibbons and Savin variants beyond what the monotone theorem implies. parent of this event

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De Giorgi's conjecture on monotone solutions of the Allen-Cahn equation — Mathematical Frontier Network