Long-time behavior of solutions to the generalized Allen-Cahn model with degenerate diffusivity

preprint2020arXivOpen access

Abstract

The generalized Allen-Cahn equation, ut=ε2(D(u)ux)x−ε22D′(u)ux2−F′(u), u_t=\varepsilon^2(D(u)u_x)_x-\frac{\varepsilon^2}2D'(u)u_x^2-F'(u), with nonlinear diffusion, D=D(u)D = D(u), and potential, F=F(u)F = F(u), of the form D(u)=∣1−u2∣m,orD(u)=∣1−u∣m,m>1, D(u) = |1-u^2|^{m}, \quad \text{or} \quad D(u) = |1-u|^{m}, \quad m >1, and F(u)=12n∣1−u2∣n,n≥2, F(u)=\frac{1}{2n}|1-u^2|^{n}, \qquad n\geq2, respectively, is studied. These choices correspond to a reaction function that can be derived from a double well potential, and to a generalized degenerate diffusivity coefficient depending on the density uu that vanishes at one or at the two wells, u=±1u = \pm 1. It is shown that interface layer solutions that are equal to ±1\pm 1 except at a finite number of thin transitions of width ε\varepsilon persist for an either exponentially or algebraically long time, depending upon the interplay between the exponents nn and mm. For that purpose, energy bounds for a renormalized effective energy potential of Ginzburg-Landau type are derived.

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