Well-posedness, regularity and asymptotic analyses for a fractional phase field system

TL;DR

This paper establishes well-posedness, regularity, and long-term behavior of a fractional phase field system with complex potentials, extending classical results to fractional operators and analyzing asymptotic limits.

Contribution

It introduces a comprehensive analysis of a fractional phase field system with various potentials, extending existing well-posedness and regularity results to fractional operators and boundary conditions.

Findings

Proved well-posedness and regularity for the fractional phase field system.

Characterized the long-term behavior and stationary solutions of the system.

Demonstrated convergence to a phase relaxation problem as the fractional parameter tends to zero.

Abstract

This paper is concerned with a non-conserved phase field system of Caginalp type in which the main operators are fractional versions of two fixed linear operators $A$ and $B$. The operators $A$ and $B$ are supposed to be densely defined, unbounded, self-adjoint, monotone in the Hilbert space $L^2(\Omega)$, for some bounded and smooth domain $\Omega$, and have compact resolvents. Our definition of the fractional powers of operators uses the approach via spectral theory. A nonlinearity of double-well type occurs in the phase equation and either a regular or logarithmic potential, as well as a non-differentiable potential involving an indicator function, is admitted in our approach. We show general well-posedness and regularity results, extending the corresponding results that are known for the non-fractional elliptic operators with zero Neumann conditions or other boundary conditions like Dirichlet or Robin ones. Then, we investigate the longtime behavior of the system, by fully characterizing every element of the $\omega$-limit as a stationary solution. In the final part of the paper we study the asymptotic behavior of the system as the parameter $\sigma$ appearing in the operator $B^{2\sigma}$ that plays in the phase equation decreasingly tends to zero. We can prove convergence to a phase relaxation problem at the limit, in which an additional term containing the projection of the phase variable on the kernel of $B$ appears.