We consider the sharp interface limit for the Allen-Cahn equation and some variants in a bounded smooth domain in the case of boundary contact. The Allen-Cahn equation is a diffuse interface model since (after a short generation time) solutions typically develop so-called diffuse interfaces, where the solution stays smooth but experiences steep gradients. Moreover, the equation contains a small parameter $\varepsilon>0$ that corresponds to the thickness of the diffuse interfaces. The limit $\varepsilon\rightarrow 0$ is called \enquote{sharp interface limit} because - at least heuristically - the solutions should converge to step functions with the jump set evolving in time according to some sharp interface problem. We show the rigorous shar...
We give a short and self-contained proof for rates of convergence of the Allen--Cahn equation toward...
Diffuse and sharp interface models represent two alternatives to describe phase transitions with an ...
We consider the Allen–Cahn equation ε2∆u + u − u3 = 0 in Ω, ∂u ∂ν = 0 on ∂Ω, where Ω is a smooth ...
We consider the sharp interface limit for the Allen-Cahn equation and some variants in a bounded smo...
In this thesis we rigorously prove that the Cahn-Larché system converges to a modified Hele-Shaw pro...
We consider the sharp interface limit for the scalar-valued and vector-valued Allen–Cahn equation wi...
We discuss the sharp interface limit of a coupled Navier-Stokes/Allen-Cahn system in a two dimension...
We discuss the sharp interface limit of a diffuse interface model for a two-phase flow of two partly...
The behavior of the Allen-Cahn equation ∂ t u ε (x,t)= Δ u ε (x,t) - ε -2 F'(u ε (x,t))+ ξ ...
We consider the sharp interface limit of a coupled Stokes/Allen-Cahn system, when a parameter that i...
In this contribution, we investigate a diffuse interface model for quasi-incompressible flows. We de...
We rigorously show the sharp interface limit of a coupled Stokes/Cahn–Hilliard system in a two dimen...
In this contribution, we investigate a diffuse interface model for quasi–incompressible flows. We de...
Diffuse and sharp interface models represent two alternatives to describe phase transitions with an ...
Diffuse and sharp interface models represent two alternatives to describe phase transitions with an ...
We give a short and self-contained proof for rates of convergence of the Allen--Cahn equation toward...
Diffuse and sharp interface models represent two alternatives to describe phase transitions with an ...
We consider the Allen–Cahn equation ε2∆u + u − u3 = 0 in Ω, ∂u ∂ν = 0 on ∂Ω, where Ω is a smooth ...
We consider the sharp interface limit for the Allen-Cahn equation and some variants in a bounded smo...
In this thesis we rigorously prove that the Cahn-Larché system converges to a modified Hele-Shaw pro...
We consider the sharp interface limit for the scalar-valued and vector-valued Allen–Cahn equation wi...
We discuss the sharp interface limit of a coupled Navier-Stokes/Allen-Cahn system in a two dimension...
We discuss the sharp interface limit of a diffuse interface model for a two-phase flow of two partly...
The behavior of the Allen-Cahn equation ∂ t u ε (x,t)= Δ u ε (x,t) - ε -2 F'(u ε (x,t))+ ξ ...
We consider the sharp interface limit of a coupled Stokes/Allen-Cahn system, when a parameter that i...
In this contribution, we investigate a diffuse interface model for quasi-incompressible flows. We de...
We rigorously show the sharp interface limit of a coupled Stokes/Cahn–Hilliard system in a two dimen...
In this contribution, we investigate a diffuse interface model for quasi–incompressible flows. We de...
Diffuse and sharp interface models represent two alternatives to describe phase transitions with an ...
Diffuse and sharp interface models represent two alternatives to describe phase transitions with an ...
We give a short and self-contained proof for rates of convergence of the Allen--Cahn equation toward...
Diffuse and sharp interface models represent two alternatives to describe phase transitions with an ...
We consider the Allen–Cahn equation ε2∆u + u − u3 = 0 in Ω, ∂u ∂ν = 0 on ∂Ω, where Ω is a smooth ...