differential-equations / Elliptic PDE; Allen-Cahn equation and phase transitions

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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differential-equationsSep 26, 2026Significance 58/100Registry: unreviewed

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

Prior state unknown→proved

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 d…

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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.

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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