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A change in a stochastic system has three representations: Probabilistic, statistical, and informational: (i) is based on random variable $u(omega)totilde{u}(omega)$; this induces (ii) the probability distributions $F_u(x)to F_{tilde{u}}(x)$, $xinmathbb{R}^n$; and (iii) a change in the probability measure $mathbb{P}totilde{mathbb{P}}$ under the same observable $u(omega)$. In the informational representation a change is quantified by the Radon-Nikodym derivative $lnleft( frac{ d tilde{mathbb{P}}}{ dmathbb{P}}(omega)right)=-lnleft(frac{ d F_u}{ d F_{tilde{u}}}(x)right)$ when $x=u(omega)$. Substituting a random variable into its own density function creates a fluctuating entropy whose expectation has been given by Shannon. Informational representation of a deterministic transformation on $mathbb{R}^n$ reveals entropic and energetic terms, and the notions of configurational entropy of Boltzmann and Gibbs, and potential of mean force of Kirkwood. Mutual information arises for correlated $u(omega)$ and $tilde{u}(omega)$; and a nonequilibrium thermodynamic entropy balance equation is identified.
The existence of the typical set is key for the consistence of the ensemble formalization of statistical mechanics. We demonstrate here that the typical set can be defined and characterized for a general class of stochastic processes. This includes p
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