Convergence to equilibrium of weak solutions to the Cahn--Hilliard equation with non-degenerate mobility and singular potential
Maurizio Grasselli, Andrea Poiatti
TL;DR
This work proves that weak solutions to the Cahn–Hilliard equation with non-degenerate mobility and singular (logarithmic) potential converge to a single equilibrium in dimensions two and three, under only the assumption of a global weak solution satisfying an energy inequality. The authors introduce a robust strategy that uses a weak ω-limit in H^1, a De Giorgi-based separation on a set of times, and a Łojasiewicz–Simon framework to derive convergence without requiring finite-time regularization. They also extend the result to the Abels–Garcke–Grün CH–Navier–Stokes system with unmatched densities and viscosities, under the same minimal mobility condition, illustrating the method’s versatility. The approach yields convergence to equilibrium under analytic nonlinearity, provides uniform separation from pure phases, and delivers convergence in H^s for all s∈(0,1), offering a new tool for long-time analysis of CH-type models and related systems.
Abstract
We consider the classical initial and boundary value problem for the Cahn--Hilliard equation with non-degenerate mobility and singular (e.g., logarithmic) potential. We prove that any weak solution converges to a single equilibrium using only minimal assumptions, that is, the existence of a global weak solution which satisfies an energy inequality. This result appears to be new in the literature and also holds in the three-dimensional case, which was an open problem due to the lack of regularity results, especially when the mobility is just a continuous function. We then prove the same result for a Cahn--Hilliard-Navier--Stokes type system with unmatched densities and viscosities proposed by Abels, Garcke, and Grün (Math. Models Methods Appl. Sci. 22, 2012), always assuming a non-degenerate mobility. We expect that this novel method can be used to analyze the same issue for other models where the regularization properties of the solutions are unknown or unlikely.
