scholarly journals Large deviations for the current and tagged particle in 1D nearest-neighbor symmetric simple exclusion

2013 ◽  
Vol 41 (3A) ◽  
pp. 1461-1512 ◽  
Author(s):  
Sunder Sethuraman ◽  
S. R. S. Varadhan
Keyword(s):  
Large Deviations ◽  
Nearest Neighbor ◽  
Tagged Particle ◽  
Simple Exclusion

Poissonian approximation for the tagged particle in asymmetric simple exclusion

1996 ◽  
Vol 33 (02) ◽  
pp. 411-419
Author(s):  
P. A. Ferrari ◽  
L. R. G. Fontes
Keyword(s):  
Nearest Neighbor ◽  
Exclusion Process ◽  
Initial Distribution ◽  
Zero Range Process ◽  
Tagged Particle ◽  
In Series ◽  
Asymmetric Simple Exclusion ◽  
Net Flux ◽  
Simple Exclusion ◽  
The One

We consider the position of a tagged particle in the one-dimensional asymmetric nearest-neighbor simple exclusion process. Each particle attempts to jump to the site to its right at rate p and to the site to its left at rate q. The jump is realized if the destination site is empty. We assume p > q. The initial distribution is the product measure with density λ, conditioned to have a particle at the origin. We call X, the position at time t of this particle. Using a result recently proved by the authors for a semi-infinite zero-range process, it is shown that for all t ≧ 0, Xt = Nt − Bt + B 0 , where {N t} is a Poisson process of parameter (p – q)(1– λ) and {Bt } is a stationary process satisfying E exp (θ | B, |) < ∞ for some θ > 0. As a corollary we obtain that, properly centered and rescaled, the process {Xt } converges to Brownian motion. A previous result says that in the scale t 1/2, the position Xt is given by the initial number of empty sites in the interval (0, λt) divided by λ. We use this to compute the asymptotic covariance at time t of two tagged particles initially at sites 0 and rt. The results also hold for the net flux between two queues in a system of infinitely many queues in series.

Poissonian approximation for the tagged particle in asymmetric simple exclusion

1996 ◽  
Vol 33 (2) ◽  
pp. 411-419 ◽  
Author(s):  
P. A. Ferrari ◽  
L. R. G. Fontes
Keyword(s):  
Nearest Neighbor ◽  
Exclusion Process ◽  
Initial Distribution ◽  
Zero Range Process ◽  
Tagged Particle ◽  
In Series ◽  
Asymmetric Simple Exclusion ◽  
Net Flux ◽  
Simple Exclusion ◽  
The One

We consider the position of a tagged particle in the one-dimensional asymmetric nearest-neighbor simple exclusion process. Each particle attempts to jump to the site to its right at rate p and to the site to its left at rate q. The jump is realized if the destination site is empty. We assume p > q. The initial distribution is the product measure with density λ, conditioned to have a particle at the origin. We call X, the position at time t of this particle. Using a result recently proved by the authors for a semi-infinite zero-range process, it is shown that for all t ≧ 0, Xt = Nt − Bt + B0, where {Nt} is a Poisson process of parameter (p – q)(1– λ) and {Bt} is a stationary process satisfying E exp (θ | B, |) < ∞ for some θ > 0. As a corollary we obtain that, properly centered and rescaled, the process {Xt} converges to Brownian motion. A previous result says that in the scale t1/2, the position Xt is given by the initial number of empty sites in the interval (0, λt) divided by λ. We use this to compute the asymptotic covariance at time t of two tagged particles initially at sites 0 and rt. The results also hold for the net flux between two queues in a system of infinitely many queues in series.

First displacement time of a tagged particle in a stochastic cluster in a simple exclusion process with random slow bonds

2019 ◽  
Vol 51 (03) ◽  
pp. 717-744
Author(s):  
Adriana Uquillas ◽  
Adilson Simonis
Keyword(s):  
Poisson Process ◽  
Exclusion Process ◽  
Upper And Lower Bounds ◽  
Density Profiles ◽  
Tagged Particle ◽  
Simple Exclusion Process ◽  
Discrete Torus ◽  
Simple Exclusion ◽  
The One ◽  
Initial Measure

AbstractWe consider the nearest-neighbour simple exclusion process on the one-dimensional discrete torus $\mathbb{T}_N=\mathbb{Z}/N\mathbb{Z}$ , with random rates $c_N=\{c_{x,N}\colon x \in \mathbb{T}_N\}$ defined in terms of a homogeneous Poisson process on $\mathbb{R}$ with intensity $\lambda$ . Given a realization of the Poisson process, the jump rate along the edge $\{x,x+1\}$ is 1 if there is not any Poisson mark in $ (x,x+1) $ ; otherwise, it is $\lambda/N,\, \lambda \in( 0,1]$ . The density profile of this process with initial measure associated to an initial profile $\rho_0\colon \mathbb{R} \rightarrow [0,1]$ , evolves as the solution of a bounded diffusion random equation. This result follows from an appropriate quenched hydrodynamic limit. If $\lambda=1$ then $\rho$ is discontinuous at each Poisson mark with passage through the slow bonds, otherwise the conductance at the slow bonds decreases meaning no passage through the slow bonds in the continuum. The main results are concerned with upper and lower quenched and annealed bounds of $T_j$ , where $T_j$ is the first displacement time of a tagged particle in a stochastic cluster of size j (the cluster is defined via specific macroscopic density profiles). It is possible to observe that when time t grows, then $\mathbb{P}\{T_j \geq t\}$ decays quadratically in both the upper and lower bounds, and falls as slow as the presence of more Poisson marks neighbouring the tagged particle, as expected.

scholarly journals Mapping current and activity fluctuations in exclusion processes: consequences and open questions

2021 ◽  
Vol 10 (2) ◽  
Author(s):  
Matthieu Vanicat ◽  
Eric Bertin ◽  
Vivien Lecomte ◽  
Eric Ragoucy
Keyword(s):  
Large Deviations ◽  
Scaling Limit ◽  
Exclusion Process ◽  
Source Model ◽  
Quantum Spin ◽  
Exclusion Processes ◽  
Dynamical Phase Transition ◽  
Markov Matrix ◽  
Asymmetric Simple Exclusion ◽  
Simple Exclusion

Considering the large deviations of activity and current in the Asymmetric Simple Exclusion Process (ASEP), we show that there exists a non-trivial correspondence between the joint scaled cumulant generating functions of activity and current of two ASEPs with different parameters. This mapping is obtained by applying a similarity transform on the deformed Markov matrix of the source model in order to obtain the deformed Markov matrix of the target model. We first derive this correspondence for periodic boundary conditions, and show in the diffusive scaling limit (corresponding to the Weakly Asymmetric Simple Exclusion Processes, or WASEP) how the mapping is expressed in the language of Macroscopic Fluctuation Theory (MFT). As an interesting specific case, we map the large deviations of current in the ASEP to the large deviations of activity in the SSEP, thereby uncovering a regime of Kardar--Parisi--Zhang in the distribution of activity in the SSEP. At large activity, particle configurations exhibit hyperuniformity [Jack et al., PRL 114, 060601 (2015)]. Using results from quantum spin chain theory, we characterize the hyperuniform regime by evaluating the small wavenumber asymptotic behavior of the structure factor at half-filling. Conversely, we formulate from the MFT results a conjecture for a correlation function in spin chains at any fixed total magnetization (in the thermodynamic limit). In addition, we generalize the mapping to the case of two open ASEPs with boundary reservoirs, and we apply it in the WASEP limit in the MFT formalism. This mapping also allows us to find a symmetry-breaking dynamical phase transition (DPT) in the WASEP conditioned by activity, from the prior knowledge of a DPT in the WASEP conditioned by the current.

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