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The crossover regime for the weakly asymmetric simple exclusion process
Statistical Mechanics · Submitted 9 Feb 2010
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim For this parameter window we obtain the limiting distribution function of the integrated current in terms of an integral over the difference of two Fredholm determinants.
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The abstract, sentence by sentence
We consider the asymmetric simple exclusion process in one dimension with weak asymmetry (WASEP) and 0-1 step initial condition. Our interest are the fluctuations of the time-integrated particle current at some prescribed spatial location. One expects a crossover from Gaussian to Tracy-Widom distributed fluctuations. The appropriate crossover scale is an asymmetry of order $\epsilon^{-1/2}$, times of order $\epsilon^{-2}$, and a spatial location of order $\epsilon^{-3/2}$. For this parameter window we obtain the limiting distribution function of the integrated current in terms of an integral over the difference of two Fredholm determinants. For large times, on the scale $\epsilon^{-2}$, this distribution function converges to the one of Tracy-Widom.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We consider the asymmetric simple exclusion process in one dimension with weak asymmetry (WASEP) and 0-1 step initial condition. | background 0.78 | 0.43 | 0.03 | asserted 0.78 |
| s1 | Our interest are the fluctuations of the time-integrated particle current at some prescribed spatial location. | contribution 0.63 | 0.28 | 0.03 | asserted 0.92 |
| s2 | One expects a crossover from Gaussian to Tracy-Widom distributed fluctuations. | background 0.96 | 0.06 | 0.13 | hedged possibility 0.89 |
| s3 | The appropriate crossover scale is an asymmetry of order $\epsilon^{-1/2}$, times of order $\epsilon^{-2}$, and a spatial location of order $\epsilon^{-3/2}$. | result 0.76 | 0.28 | 0.23 | asserted 1.00 |
| s4 | For this parameter window we obtain the limiting distribution function of the integrated current in terms of an integral over the difference of two Fredholm determinants. | result 0.98 | 0.94 | 0.67 | asserted 1.00 |
| s5 | For large times, on the scale $\epsilon^{-2}$, this distribution function converges to the one of Tracy-Widom. | result 0.98 | 0.85 | 0.27 | asserted 1.00 |
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The paper
Original abstract
We consider the asymmetric simple exclusion process in one dimension with weak asymmetry (WASEP) and 0-1 step initial condition. Our interest are the fluctuations of the time-integrated particle current at some prescribed spatial location. One expects a crossover from Gaussian to Tracy-Widom distributed fluctuations. The appropriate crossover scale is an asymmetry of order $\epsilon^{-1/2}$, times of order $\epsilon^{-2}$, and a spatial location of order $\epsilon^{-3/2}$. For this parameter window we obtain the limiting distribution function of the integrated current in terms of an integral over the difference of two Fredholm determinants. For large times, on the scale $\epsilon^{-2}$, this distribution function converges to the one of Tracy-Widom.
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How the literature uses it
5 arXiv papers cite this in 8 sentences
Papers citing it · 6 sentences without a confident label
Cites it as background 2 papers
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A more detailed exposition can be found in [ref] .
The one-dimensional KPZ equation: an exact solution and its universality · Introduction · 0.89
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Exact results have also been obtained for the KPZ equation itself, and its equivalent system, the continuous directed polymer [ref] .
Half-space stationary Kardar-Parisi-Zhang equation · Introduction · 0.83
What it cites · 3 sentences without a confident label
Compares with 1 paper
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Corwin, and J. Quastel posted their paper [ref] in the arXiv, in which independently they establish the limit ([ref]) and the formula ([ref]) for the probability density $ρ_t$.
Probability Distribution of the Free Energy of the Continuum Directed Random Polymer in 1+1 dimensions · Conclusions · 0.92
Cites as background 1 paper
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Properties of this family of distribution functions and their relation to the KPZ equation will be discussed in the companion papers [ref] .
Exact height distributions for the KPZ equation with narrow wedge initial condition · Conclusions · 0.87
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