Current preprints by Lorenzo Bertini
- L. Bertini, G. Di Gesù
Small noise asymptotic of the Gallavotti-Cohen functional for
diffusion processes
Abstract.
We consider, for a diffusion process in $\bb R^n$, the
Gallavotti-Cohen functional, defined as the empirical power dissipated
in a time interval by the non-conservative part of the drift. We
prove a large deviation principle in the limit in which the noise
vanishes and the time interval diverges. The corresponding rate
functional, which satisfies the fluctuation theorem, is expressed in
terms of a variational problem on the classical Freidlin-Wentzell
functional.
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- L. Bertini, M. Ponsiglione
A variational approach to the stationary solutions of Burgers equation
Abstract.
Consider the viscous Burgers equation on a bounded interval with
inhomogeneous Dirichlet boundary conditions. Following the
variational framework introduced by Bertini et al., we analyze a
Lyapunov functional for such equation which gives the large deviations
asymptotics of a stochastic interacting particles model associated to
the Burgers equation. We discuss the asymptotic behavior of this
energy functional, whose minimizer is given by the unique stationary
solution, as the length of the interval diverges. We focus on
boundary data corresponding to a standing wave solution to the Burgers
equation in the whole line. In this case, the limiting functional has
in fact a one-parameter family of minimizers and we analyze the
so-called development by Γ-convergence; this amounts to compute
the sharp asymptotic cost corresponding to a given shift of the
stationary solution.
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- L. Bertini, A. Faggionato, D. Gabrielli
Large deviation principles for non gradient weakly asymmetric
stochastic lattice gases
Abstract.
We consider a lattice gas on the discrete $d$-dimensional torus $(\bb
Z/N \bb Z)^d$ with a generic translation invariant, finite range
interaction satisfying a uniform strong mixing condition. The
lattice gas performs a Kawasaki dynamics in the presence of a weak
external field $E/N$. We show that, under diffusive rescaling, the
hydrodynamic behavior of the lattice gas is described by a nonlinear
driven diffusion equation. We then prove the associated dynamical
large deviation principle. Under suitable assumptions on the
external field (e.g. $E$ constant), we finally analyze the
variational problem defining the quasi-potential and characterize
the optimal exit trajectory. From these results we deduce the
asymptotic behavior of the stationary measures of the stochastic
lattice gas, which are not explicitly known. In particular, when the
external field $E$ is constant, we prove a stationary large
deviation principle for the empirical density and show that the rate
function does not depend on $E$.
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file.
-
L. Bertini, P. Buttà, A. Garroni
Boundary effects in the gradient theory of phase transitions
Abstract.
We consider the van der Waals' free energy functional, with scaling
parameter $\epsilon$, in the plane domain $\mathbb{R}_+\times
\mathbb{R}_+$, with inhomogeneous Dirichlet boundary conditions. We
impose the two stable phases on the horizontal boundaries
$\mathbb{R}_+ \times\{0\}$ and $\mathbb{R}_+\times\{\infty\}$,
and free boundary conditions on $\{\infty\}\times\mathbb{R}_+$.
Finally, the datum on $\{0\}\times \mathbb{R}_+$ is chosen in such a way
that the interface between the pure phases is pinned at some point
$(0,y)$. We show that there exists a critical scaling, $y=y_\epsilon$,
such that, as $\epsilon\to 0$, the competing effects of repulsion from the
boundary and penalization of gradients play a role in determining the
optimal shape of the (properly rescaled) interface. This result is
achieved by means of an asymptotic development of the free energy
functional. As a consequence, such analysis is not restricted to
minimizers but also encodes the asymptotic probability of
fluctuations.
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-
L. Bertini, N. Cancrini, G. Posta
On the dynamical behavior of the ABC model
Abstract.
We consider the ABC dynamics, with equal density of the three species,
on the discrete ring with $N$ sites.
In this case, the process is reversible with respect to a Gibbs measure
with a mean field interaction that undergoes a second order phase
transition.
We analyze the relaxation time of the dynamics and show that at high
temperature it grows at most as $N^2$ while it grows at least as
$N^3$ at low temperature.
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file.
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