AbstractWe study a generalization of the fully overdamped Frenkel–Kontorova model in dimension n⩾1. This model describes the evolution of the position of each atom in a crystal, and is mathematically given by an infinite system of coupled first order ODEs. We prove that for a suitable rescaling of this model, the solution converges to the solution of a Peierls–Nabarro model, which is a coupled system of two PDEs (typically an elliptic PDE in a domain with an evolution PDE on the boundary of the domain). This passage from the discrete model to a continuous model is done in the framework of viscosity solutions
n this paper a phase-field model of Penrose-Fife type is considered for diffusive phase transitions ...
The system of partial differential equations -div (vDu) = f in Q vertical bar Du vertical bar - 1 = ...
AbstractWe study the multiplicity of nonnegative solutions to the problem,(Pλ)−Δu=λa(x)up+f(u)inΩ,u=...
We study a generalization of the fully overdamped Frenkel-Kontorova model in dimension $n\geq 1.$ Th...
AbstractWe study a generalization of the fully overdamped Frenkel–Kontorova model in dimension n⩾1. ...
We consider an evolution equation arising in the Peierls--Nabarro model for crystal dislocation. we ...
AbstractIn this paper, we consider the fully overdamped Frenkel–Kontorova model. This is an infinite...
AbstractThis paper is concerned with a result of homogenization of an integro-differential equation ...
We consider a reaction-diffusion equation with a half-Laplacian. In the case where the solution is i...
We consider an evolution equation arising in the Peierls-Nabarro model for crystal dislocation. We s...
AbstractIn this work, we consider a general fully overdamped Frenkel–Kontorova model. This model des...
International audienceIn this paper, we consider the fully overdamped Frenkel-Kontorova model. This ...
AbstractWe consider the full nonlinear dynamic von Kármán system of equations which models large def...
AbstractAn intimate connection between the Peierls–Nabarro equation in crystal-dislocation theory an...
International audienceIn this work, we consider a general fully overdamped Frenkel-Kontorova model. ...
n this paper a phase-field model of Penrose-Fife type is considered for diffusive phase transitions ...
The system of partial differential equations -div (vDu) = f in Q vertical bar Du vertical bar - 1 = ...
AbstractWe study the multiplicity of nonnegative solutions to the problem,(Pλ)−Δu=λa(x)up+f(u)inΩ,u=...
We study a generalization of the fully overdamped Frenkel-Kontorova model in dimension $n\geq 1.$ Th...
AbstractWe study a generalization of the fully overdamped Frenkel–Kontorova model in dimension n⩾1. ...
We consider an evolution equation arising in the Peierls--Nabarro model for crystal dislocation. we ...
AbstractIn this paper, we consider the fully overdamped Frenkel–Kontorova model. This is an infinite...
AbstractThis paper is concerned with a result of homogenization of an integro-differential equation ...
We consider a reaction-diffusion equation with a half-Laplacian. In the case where the solution is i...
We consider an evolution equation arising in the Peierls-Nabarro model for crystal dislocation. We s...
AbstractIn this work, we consider a general fully overdamped Frenkel–Kontorova model. This model des...
International audienceIn this paper, we consider the fully overdamped Frenkel-Kontorova model. This ...
AbstractWe consider the full nonlinear dynamic von Kármán system of equations which models large def...
AbstractAn intimate connection between the Peierls–Nabarro equation in crystal-dislocation theory an...
International audienceIn this work, we consider a general fully overdamped Frenkel-Kontorova model. ...
n this paper a phase-field model of Penrose-Fife type is considered for diffusive phase transitions ...
The system of partial differential equations -div (vDu) = f in Q vertical bar Du vertical bar - 1 = ...
AbstractWe study the multiplicity of nonnegative solutions to the problem,(Pλ)−Δu=λa(x)up+f(u)inΩ,u=...