We present a quenched weak large deviations principle for the Gibbs measures of a Random Field Kac Model (RFKM) in one dimension. The external random magnetic field is given by symmetrically distributed Bernouilli random variables. The results are valid for values of the temperature and magnitude of the field in the region where the free energy of the corresponding random Curie Weiss model has only two absolute minimizers. We give an explicit representation of the large deviation rate function and characterize its minimizers. We show that they are step functions taking two values, the two absolute minimizers of the free energy of the random Curie Weiss model. The points of discontinuity...
We review our recent results on the low temperature behavior of Kac models. We discuss translation-i...
We analyze the dynamics of moderate fluctuations for macroscopic observables of the random field Cur...
We consider the Kac-Ising model in an arbitrary configuration of local magnetic fields η = (ηi)i∈Zd,...
We present a quenched weak large deviations principle for the Gibbs measures of a Random Field K...
We study a spin-flip model with Kac type interaction, in the presence of a random field given by i.i...
40 pagesInternational audienceWe study a spin-flip model with Kac type interaction, in the presence ...
We consider the Kac-Ising model in an arbitrary configuration of local magnetic fields η = (ηi)i∈Zd,...
We consider the Kac–Ising model in an arbitrary configuration of local magnetic fields η=(ηi)i ∈ Zd,...
AbstractWe consider a Langevin dynamics scheme for a d-dimensional Ising model with a disordered ext...
We consider a lattice gas in a periodic $d-$ dimensional lattice of width $\g^{-1}$, $\g>0$, inter...
We study the typical profiles of a one dimensional random fieldKac model, for values of the temperat...
Abstract. Let X = {Xt}t∈Zd ∼ P and Y = {Yt}t∈Zd ∼ Q be two independent stationary random fields with...
We review our recent results on the low temperature behavior of Kac models. We discuss translation-i...
We prove that the Large Deviation Principle holds for the distribution of the particle number densit...
We review our recent results on the low temperature behavior of Kac models. We discuss translation-i...
We review our recent results on the low temperature behavior of Kac models. We discuss translation-i...
We analyze the dynamics of moderate fluctuations for macroscopic observables of the random field Cur...
We consider the Kac-Ising model in an arbitrary configuration of local magnetic fields η = (ηi)i∈Zd,...
We present a quenched weak large deviations principle for the Gibbs measures of a Random Field K...
We study a spin-flip model with Kac type interaction, in the presence of a random field given by i.i...
40 pagesInternational audienceWe study a spin-flip model with Kac type interaction, in the presence ...
We consider the Kac-Ising model in an arbitrary configuration of local magnetic fields η = (ηi)i∈Zd,...
We consider the Kac–Ising model in an arbitrary configuration of local magnetic fields η=(ηi)i ∈ Zd,...
AbstractWe consider a Langevin dynamics scheme for a d-dimensional Ising model with a disordered ext...
We consider a lattice gas in a periodic $d-$ dimensional lattice of width $\g^{-1}$, $\g>0$, inter...
We study the typical profiles of a one dimensional random fieldKac model, for values of the temperat...
Abstract. Let X = {Xt}t∈Zd ∼ P and Y = {Yt}t∈Zd ∼ Q be two independent stationary random fields with...
We review our recent results on the low temperature behavior of Kac models. We discuss translation-i...
We prove that the Large Deviation Principle holds for the distribution of the particle number densit...
We review our recent results on the low temperature behavior of Kac models. We discuss translation-i...
We review our recent results on the low temperature behavior of Kac models. We discuss translation-i...
We analyze the dynamics of moderate fluctuations for macroscopic observables of the random field Cur...
We consider the Kac-Ising model in an arbitrary configuration of local magnetic fields η = (ηi)i∈Zd,...