Clifford Tori and the singularly perturbed Cahn-Hilliard equation

preprint2015arXivOpen access

Abstract

In this paper we construct entire solutions uεu_{\varepsilon} to the Cahn-Hilliard equation −ε2Δ(−ε2Δu+W′(u))+W"(u)(−ε2Δu+W′(u))=0-\varepsilon^{2}Δ(-\varepsilon^{2}Δu+W^{'}(u))+W^{"}(u)(-\varepsilon^{2}Δu+W^{'}(u))=0, under the volume constraint ∫R3(1−uε)dx=42π2\int_{\mathbb{R}^{3}}(1-u_{\varepsilon})dx=4\sqrt{2}π^{2}, whose nodal set approaches the Clifford Torus, that is the Torus with radii of ratio 1/21/\sqrt{2} embedded in R3\mathbb{R}^{3}, as ε→0\varepsilon\to 0. What is crucial is that the Clifford Torus is a Willmore hypersurface and it is non-degenerate, up to conformal transformations. The proof is based on the Lyapunov-Schmidt reduction and on careful geometric expansions of the laplacian.

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