2016
DOI: 10.1007/s00285-016-0980-x
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A multi-time-scale analysis of chemical reaction networks: II. Stochastic systems

Abstract: We consider stochastic descriptions of chemical reaction networks in which there are both fast and slow reactions, and for which the time scales are widely separated. We develop a computational algorithm that produces the generator of the full chemical master equation for arbitrary systems, and show how to obtain a reduced equation that governs the evolution on the slow time scale. This is done by applying a state space decomposition to the full equation that leads to the reduced dynamics in terms of certain p… Show more

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Cited by 23 publications
(19 citation statements)
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“…Other approaches due to Haseltine and Rawlings [18] and Goutsias [19] model the state of the system using extents of reaction as opposed to molecules of species. A singular perturbation theory based method has also recently been used to obtain a reduced stochastic description [20].…”
Section: Introductionmentioning
confidence: 99%
“…Other approaches due to Haseltine and Rawlings [18] and Goutsias [19] model the state of the system using extents of reaction as opposed to molecules of species. A singular perturbation theory based method has also recently been used to obtain a reduced stochastic description [20].…”
Section: Introductionmentioning
confidence: 99%
“…Property 2 suggests, but does not provide a definitive proof, that the distribution of X is Poissonian if ε = 0 or δ = 0. In the non-interaction case (δ = 0), the proof is straightforward: the dynamics of X is that of a simple immigrationand-death process, which is known to generate a Poisson distribution [47][48][49]. If X is stable (ε = 0), the distribution is again Poisson, but the proof requires a more subtle reasoning based on the Chemical Reaction Network Theory.…”
Section: The Statement Of the Model And Main Resultsmentioning
confidence: 99%
“…where y i L α i is the forward operator of the catalysed network R α i , while L β of the uncatalysed network R β . The forward operator from (25) is singularly perturbed, and, in what follows, we apply perturbation theory to exploit this fact [23,27]. Substituting the power series expansion p(x, y, τ ) = p 0 (x, y, τ ) + ε p 1 (x, y, τ ) + .…”
Section: Stochastic Analysismentioning
confidence: 99%