Emergence of jams in the generalized totally asymmetric simple exclusion process

被引:17
作者
Derbyshev, A. E. [1 ,2 ]
Povolotsky, A. M. [1 ,3 ]
Priezzhev, V. B. [1 ]
机构
[1] Joint Inst Nucl Res, Bogoliubov Lab Theoret Phys, Dubna 141980, Russia
[2] Moscow Inst Phys & Technol, Dolgoprudnyi, Russia
[3] NRU HSE, Phys Math Lab, Moscow, Russia
来源
PHYSICAL REVIEW E | 2015年 / 91卷 / 02期
关键词
LARGE-DEVIATION FUNCTION; BETHE-ANSATZ SOLUTION; PHASE-TRANSITIONS; MODELS; DYNAMICS; EQUATION; SURFACE; TASEP;
D O I
10.1103/PhysRevE.91.022125
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
The generalized totally asymmetric exclusion process (TASEP) [J. Stat. Mech. (2012) P05014] is an integrable generalization of the TASEP equipped with an interaction, which enhances the clustering of particles. The process interpolates between two extremal cases: the TASEP with parallel update and the process with all particles irreversibly merging into a single cluster moving as an isolated particle. We are interested in the large time behavior of this process on a ring in the whole range of the parameter. controlling the interaction. We study the stationary state correlations, the cluster size distribution, and the large-time fluctuations of integrated particle current. When. is finite, we find the usual TASEP-like behavior: The correlation length is finite; there are only clusters of finite size in the stationary state and current fluctuations belong to the Kardar-Parisi-Zhang universality class. When. grows with the system size, so does the correlation length. We find a nontrivial transition regime with clusters of all sizes on the lattice. We identify a crossover parameter and derive the large deviation function for particle current, which interpolates between the case considered by Derrida-Lebowitz and a single-particle diffusion.
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页数:16
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