2006
DOI: 10.1088/0305-4470/39/29/004
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Exact solution and asymptotic behaviour of the asymmetric simple exclusion process on a ring

Abstract: In this paper, we study an exact solution of the asymmetric simple exclusion process on a periodic lattice of finite sites with two typical updates, i.e., random and parallel. Then, we find that the explicit formulas for the partition function and the average velocity are expressed by the Gauss hypergeometric function. In order to obtain these results, we effectively exploit the recursion formula for the partition function for the zero-range process. The zero-range process corresponds to the asymmetric simple … Show more

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Cited by 28 publications
(34 citation statements)
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“…In this paper, we focus on probabilistic extension of BCA (PBCA). It is partially equivalent to the 'totally' ASEP (TASEP) obtained by restricting the motion of particles of ASEP to the only one direction [8,9,10]. However, there is a difference between PBCA and TASEP about the updating way of particle positions.…”
Section: Introductionmentioning
confidence: 99%
“…In this paper, we focus on probabilistic extension of BCA (PBCA). It is partially equivalent to the 'totally' ASEP (TASEP) obtained by restricting the motion of particles of ASEP to the only one direction [8,9,10]. However, there is a difference between PBCA and TASEP about the updating way of particle positions.…”
Section: Introductionmentioning
confidence: 99%
“…It is rather difficult, however, to define parallel update dynamics for a system with an infinite number of particles, since the number of updated sites can be infinity, i.e., | A t | = ∞ using the notation in Sec.I. Kanai et al [10] overcame this difficulty and determined the thermodynamic limit of average velocity (13). They obtained the differential equation which governs the average velocity and took the thermodynamic limit in the equation.…”
Section: Discussionmentioning
confidence: 99%
“…are assumed to be functions of p and ρ. Putting (33) and (34) into (30) and its modification obtained by setting L → L − 1, and taking the thermodynamic limit K → ∞ with ρ = L/K = const., the first terms in (33) and (34) are determined as [10] v…”
Section: A Riccati Equationsmentioning
confidence: 99%
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“…The average velocity is then given using random sequential update rule as ω avg = ω 2 . J ρ N = ω 2 .p(1 − ρ N ) [13][14][15], where J is the average current in the system, p = f sb and ω 2 is the normalization constant. Inset of Fig.…”
mentioning
confidence: 99%