Stationary measures for an exclusion process on one-dimensional lattices with infinitely many hopping sites (Q1820518)
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scientific article; zbMATH DE number 3996824
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Stationary measures for an exclusion process on one-dimensional lattices with infinitely many hopping sites |
scientific article; zbMATH DE number 3996824 |
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Stationary measures for an exclusion process on one-dimensional lattices with infinitely many hopping sites (English)
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1986
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Stationary measures for the following exclusion process on one- dimensional lattices with discrete time parameter are considered: As time increases from t to \(t+1\), each particle which locates at the site i moves to the site i-1 independently with probability \(\alpha\) \((0<\alpha <1/2)\) iff the site i-1 is unoccupied. It is known that the stationary measures for the process are the convex combinations of a family of nearest neighbor Gibbs states (renewal measures) \(\{\pi_{\gamma}:\) \(0<\gamma <\infty \}\) and trivial Dirac measures \(\{\pi_ 0,\pi_{\infty},\Theta_ n,n\in {\mathbb{Z}}\}\). Concerning the stochastic property of a tagged particle under the time evolution with respect to the stationary state \(\pi_{\gamma}\), it is shown that the position of tagged particle \(\{\) r(t), \(t=0,1,2,...\}\) has independent increments, i.e., \(\{\) r(t)-r(t-1)\(\}\) is a Bernoulli sequence, and so a central limit theorem holds. By applying a simple limiting procedure to our process we can obtain a usual simple exclusion process with continuous time parameter.
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infinite particle systems
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Gibbs states
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Dirac measures
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tagged particle
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central limit theorem
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exclusion process
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0.92227006
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0.9079655
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0.90034074
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0.8932501
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0.8897358
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0.8880964
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