Markov trajectories : Microcanonical Ensembles based on empirical observables as compared to Canonical Ensembles based on Markov generators
arXiv:2201.00666 · doi:10.1140/epjb/s10051-022-00386-x
Abstract
The Ensemble of trajectories produced by the Markov generator can be considered as 'Canonical' for the following reasons : (C1) the probability of the trajectory can be rewritten as the exponential of a linear combination of its relevant empirical time-averaged observables , where the coefficients involving the Markov generator are their fixed conjugate parameters; (C2) the large deviations properties of these empirical observables for large are governed by the explicit rate function at Level 2.5, while in the thermodynamic limit , they concentrate on their typical values determined by the Markov generator . This concentration property in the thermodynamic limit suggests to introduce the notion of the 'Microcanonical Ensemble' at Level 2.5 for stochastic trajectories , where all the relevant empirical variables are fixed to some values and cannot fluctuate anymore for finite . The goal of the present paper is to discuss its main properties : (MC1) when the long trajectory belongs the Microcanonical Ensemble with the fixed empirical observables , the statistics of its subtrajectory for is governed by the Canonical Ensemble associated to the Markov generator that would make the empirical observables typical ; (MC2) in the Microcanonical Ensemble, the central role is played by the number of stochastic trajectories of duration with the given empirical observables , and by the corresponding explicit Boltzmann entropy . This general framework is applied to continuous-time Markov Jump processes and to discrete-time Markov chains with illustrative examples.
arXiv commentv2 : final version (33 pages)
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