2012
DOI: 10.1088/1751-8113/45/46/465004
|View full text |Cite
|
Sign up to set email alerts
|

Long time asymptotics of the totally asymmetric simple exclusion process

Abstract: We study the long time asymptotics of the relaxation dynamics of the totally asymmetric simple exclusion process on a ring. Evaluating the asymptotic amplitudes of the local currents by the algebraic Bethe ansatz method, we find the relaxation times starting from the step and alternating initial conditions are governed by different eigenvalues of the Markov matrix. In both cases, the scaling exponents of the leading asymptotic amplitudes with respect to the total number of sites are found to be −1. We also stu… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

1
24
0

Year Published

2013
2013
2020
2020

Publication Types

Select...
6

Relationship

1
5

Authors

Journals

citations
Cited by 12 publications
(25 citation statements)
references
References 46 publications
1
24
0
Order By: Relevance
“…The expression (4) follows directly from that of the generating function e sh(x,t) flat , s > 0 obtained in [39], equation (8) S , based on earlier works [44,85,86,87,54,45,88,53] on the Bethe ansatz solution of TASEP with periodic boundaries. One has e sh(x,t)…”
Section: Relation With the Generating Function Of The Heightmentioning
confidence: 99%
“…The expression (4) follows directly from that of the generating function e sh(x,t) flat , s > 0 obtained in [39], equation (8) S , based on earlier works [44,85,86,87,54,45,88,53] on the Bethe ansatz solution of TASEP with periodic boundaries. One has e sh(x,t)…”
Section: Relation With the Generating Function Of The Heightmentioning
confidence: 99%
“…The derivative with respect to y i in the determinant has to be computed before setting the y j 's equal to a solution of the Bethe equations (4). At q = 0, the determinant can be calculated explicitly [25], which allows the asymptotic analysis for large L, N [26]. The Gaudin determinant is a consequence of the Slavnov determinant [27] for the scalar product between a Bethe eigenstate ψ y with Bethe roots y j and a Bethe vector ψ w with arbitrary parameters w j not solution of Bethe equations,…”
Section: Scalar Product Of Bethe Eigenstatesmentioning
confidence: 99%
“…This fact allows us to determine the factor K by evaluating the overlap for a particular particle configuration. In fact, the overlaps for some particular cases can be directly evaluated as in [30,31]. For instance, we find the following explicit expression for the case x j = j (1 ≤ j ≤ n):…”
Section: (J)mentioning
confidence: 99%
“…On the other hand, the overall factor is independent of the particle positions, and therefore we can determine this factor by considering the specific configuration: we explicitly calculate it with the help of the result for the overlap of the consecutive configuration (i.e. x j = j) obtained in [30,31].…”
Section: Wavefunctionsmentioning
confidence: 99%
See 1 more Smart Citation