2009
DOI: 10.1088/1742-5468/2009/05/p05014
|View full text |Cite
|
Sign up to set email alerts
|

Exact matrix-product states for parallel dynamics: open boundaries and excess mass on the ring

Abstract: Abstract. In this paper it is shown that the steady-state weights of the asymmetric simple exclusion process (ASEP) with open boundaries and parallel update can be written as a product of a scalar pair-factorized and a matrix-product state. This type of state is also obtained for an ASEP on a ring in which particles can move one or two sites. The dynamics leads to the formation of an excess hole that plays the role of a defect. We expect the process to play a similar role for parallel dynamics as the well-know… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1

Citation Types

0
47
0

Year Published

2010
2010
2020
2020

Publication Types

Select...
5
1

Relationship

2
4

Authors

Journals

citations
Cited by 13 publications
(47 citation statements)
references
References 24 publications
0
47
0
Order By: Relevance
“…In the parallel update [116,324,392], all sites are updated at the same time. The state of a given site at time t + 1 depends on the state of this site and its neighbors at time t, through -when applied to the TASEP-the rules introduced in section 4.1.1.…”
Section: Update Schemementioning
confidence: 99%
“…In the parallel update [116,324,392], all sites are updated at the same time. The state of a given site at time t + 1 depends on the state of this site and its neighbors at time t, through -when applied to the TASEP-the rules introduced in section 4.1.1.…”
Section: Update Schemementioning
confidence: 99%
“…Reference [18] gives a review of parallel TASEP on a ring with a focus on traffic applications. More recently, the steady-state of a parallel TASEP on a ring where particles can jump one or two sites ahead has been characterised as a scalar-pair factorised and a matrix-product state [22].…”
Section: Introductionmentioning
confidence: 99%
“…with q = 1 − p. In this paper we interpret W ({τ }) as the number of particle-hole domain walls in the configuration {τ }. This is one possible choice following [13]. Again the vectors W | and |V reflect the boundaries and the matrices D and E represent particles and holes respectively but are different from those for the random-sequential case.…”
Section: The Tasep and The Matrix Ansatzmentioning
confidence: 99%