Negative Entropy, Zero temperature and stationary Markov Chains on the interval
| dc.creator | Lopes, Artur O. | |
| dc.creator | Mohr, Joana | |
| dc.creator | Souza, Rafael R. | |
| dc.creator | Thieullen, Philippe | |
| dc.date | 2008-06-05 | |
| dc.date | 2009-01-06 | |
| dc.date.accessioned | 2026-07-07T12:24:17Z | |
| dc.date.available | 2026-07-07T12:24:17Z | |
| dc.description | We analyze some properties of maximizing stationary Markov probabilities on the Bernoulli space $[0,1]^\mathbb{N}$, More precisely, we consider ergodic optimization for a continuous potential $A$, where $A: [0,1]^\mathbb{N}\to \mathbb{R}$ which depends only on the two first coordinates. We are interested in finding stationary Markov probabilities $μ_\infty$ on $ [0,1]^\mathbb{N}$ that maximize the value $ \int A d μ,$ among all stationary Markov probabilities $μ$ on $[0,1]^\mathbb{N}$. This problem correspond in Statistical Mechanics to the zero temperature case for the interaction described by the potential $A$. The main purpose of this paper is to show, under the hypothesis of uniqueness of the maximizing probability, a Large Deviation Principle for a family of absolutely continuous Markov probabilities $μ_β$ which weakly converges to $μ_\infty$. The probabilities $μ_β$ are obtained via an information we get from a Perron operator and they satisfy a variational principle similar to the pressure. Under the hypothesis of $A$ being $C^2$ and the twist condition, that is, $\frac{\partial^2 A}{\partial_x \partial_y} (x,y) \neq 0$, for all $(x,y) \in [0,1]^2$, we show the graph property. | |
| dc.identifier | https://arxiv.org/abs/0806.1012 | |
| dc.identifier | http://arxiv.org/abs/0806.1012 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/214275 | |
| dc.subject | Dynamical Systems | |
| dc.subject | Probability | |
| dc.subject | 37A35; 37A50; 37A60; 60J10 | |
| dc.title | Negative Entropy, Zero temperature and stationary Markov Chains on the interval | |
| dc.type | text |