2000
DOI: 10.1103/physreve.61.2300
|View full text |Cite
|
Sign up to set email alerts
|

Exact results for a fully asymmetric exclusion process with sequential dynamics and open boundaries

Abstract: An exact and rigorous calculation of the current and density profile in the steady state of the one-dimensional fully asymmetric simple-exclusion process with open boundaries and forward-ordered sequential dynamics is presented. The method is based on a matrix product representation of the steady-state probability distribution. The main idea is to choose a suitable representation in which the scalar products describing the current and local density profile for a chain of arbitrary finite size depend only on th… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

0
23
0

Year Published

2000
2000
2011
2011

Publication Types

Select...
5
4

Relationship

1
8

Authors

Journals

citations
Cited by 18 publications
(23 citation statements)
references
References 11 publications
0
23
0
Order By: Relevance
“…A), e.g. random-sequential [167,168], ordered-sequential [166,169,170] and sublattice-parallel update [171][172][173]166]. One finds that the phase diagram has the same basic structure for all updates [166].…”
Section: Exact Solution Of the Nasch Model With V Max = 1 And Open Bomentioning
confidence: 99%
“…A), e.g. random-sequential [167,168], ordered-sequential [166,169,170] and sublattice-parallel update [171][172][173]166]. One finds that the phase diagram has the same basic structure for all updates [166].…”
Section: Exact Solution Of the Nasch Model With V Max = 1 And Open Bomentioning
confidence: 99%
“…Finally the phase diagram for forward ordered updating can be obtained from the particle-hole symmetry mentioned above. Current and density profiles have been calculated in [179,180].…”
Section: Ordered Sequential Dynamicsmentioning
confidence: 99%
“…Next, the method of MPA was successfully applied for obtaining the steady-state properties in all the basic cases of true discrete-time dynamics: forward-(→) and backward-ordered (←) sequential [8], [9], [10], sublattice-parallel (s-) [11], [12], and, finally, fully parallel dynamics [13], [14].…”
Section: Introductionmentioning
confidence: 99%
“…The coexistence line between the low-and highdensity phases is given by (α = β, 0 ≤ β ≤ β c ); on crossing it the bulk density undergoes a finite jump. Here, the exact finite-size expressions for the current and local density in the steady state of FASEP with open boundaries and forward-ordered sequential update, derived in [10], are analysed within the framework of finite-size scaling (FSS) at continuous (for the current) and first-order (for the density) phase transitions. The appropriate scaling variables are identified and the corresponding scaling functions for the current and local desity are explicitly obtained.…”
Section: Introductionmentioning
confidence: 99%