Markov trajectories : Microcanonical Ensembles based on empirical observables as compared to Canonical Ensembles based on Markov generators

Abstract

The Ensemble of trajectories x(0 ≤ t ≤ T) produced by the Markov generator M can be considered as 'Canonical' for the following reasons : (C1) the probability of the trajectory x(0 ≤ t ≤ T) can be rewritten as the exponential of a linear combination of its relevant empirical time-averaged observables En, where the coefficients involving the Markov generator are their fixed conjugate parameters; (C2) the large deviations properties of these empirical observables En for large T are governed by the explicit rate function I[2.5]M (E.) at Level 2.5, while in the thermodynamic limit T=+∞, they concentrate on their typical values Entyp[M] determined by the Markov generator M. This concentration property in the thermodynamic limit T=+∞ suggests to introduce the notion of the 'Microcanonical Ensemble' at Level 2.5 for stochastic trajectories x(0 ≤ t ≤ T), where all the relevant empirical variables En are fixed to some values E*n and cannot fluctuate anymore for finite T. The goal of the present paper is to discuss its main properties : (MC1) when the long trajectory x(0 ≤ t ≤ T) belongs the Microcanonical Ensemble with the fixed empirical observables En*, the statistics of its subtrajectory x(0 ≤ t ≤ τ) for 1 τ T is governed by the Canonical Ensemble associated to the Markov generator M* that would make the empirical observables En* typical ; (MC2) in the Microcanonical Ensemble, the central role is played by the number [2.5]T(E*.) of stochastic trajectories of duration T with the given empirical observables E*n, and by the corresponding explicit Boltzmann entropy S[2.5]( E*. ) = [ [2.5]T(E*.)]/T . This general framework is applied to continuous-time Markov Jump processes and to discrete-time Markov chains with illustrative examples.

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