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RESEARCH PRODUCT
Role of conditional probability in multiscale stationary markovian processes.
Salvatore Miccichèsubject
Continuous-time stochastic processPure mathematicsStationary processStationary distributionStatistical Mechanics (cond-mat.stat-mech)Stochastic processStochastic ProcesseFokker-Plank EquationFOS: Physical sciencesOrnstein–Uhlenbeck processConditional probability distributionSettore FIS/07 - Fisica Applicata(Beni Culturali Ambientali Biol.e Medicin)CombinatoricsStable processPhysics - Data Analysis Statistics and ProbabilityMarkovian processeFirst-hitting-time modelCondensed Matter - Statistical MechanicsData Analysis Statistics and Probability (physics.data-an)Mathematicsdescription
The aim of the paper is to understand how the inclusion of more and more time-scales into a stochastic stationary Markovian process affects its conditional probability. To this end, we consider two Gaussian processes: (i) a short-range correlated process with an infinite set of time-scales bounded from below, and (ii) a power-law correlated process with an infinite and unbounded set of time-scales. For these processes we investigate the equal position conditional probability P(x,t|x,0) and the mean First Passage Time T(L). The function P(x,t|x,0) can be considered as a proxy of the persistence, i.e. the fact that when a process reaches a position x then it spends some time around that position value. The mean First Passage Time can be considered as a proxy of how fast is the process in reaching a position at distance L starting from position x. In the first investigation we show that the more time-scales the process includes, the larger the persistence. Specifically, we show that the power-law correlated process shows a slow power-law decay of P(x,t|x,0) to the stationary pdf. By contrast, the short range correlated process shows a decay dominated by an exponential cut-off. Moreover, we also show that the existence of an infinite and unbouded set of time-scales is a necessary and not sufficient condition for observing a slow power-law decay of P(x,t|x,0). In the second investigation, we show that for large values of L the more time-scales the process includes, the larger the mean First Passage Time, i.e. the slowest the process. On the other hand, for small values of L, the more time-scales the process includes, the smaller the mean First Passage Time, i.e. when a process statistically spends more time in a given position the likelihood that it reached nearby positions by chance is also enhanced.
year | journal | country | edition | language |
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2010-01-01 | Physical review. E, Statistical, nonlinear, and soft matter physics |