2014
DOI: 10.1103/physrevlett.113.120601
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Universal Large Deviations for the Tagged Particle in Single-File Motion

Abstract: We consider a gas of point particles moving in a one-dimensional channel with a hard-core inter-particle interaction that prevents particle crossings -this is called single-file motion. Starting from equilibrium initial conditions we observe the motion of a tagged particle. It is well known that if the individual particle dynamics is diffusive, then the tagged particle motion is sub-diffusive, while for ballistic particle dynamics, the tagged particle motion is diffusive. Here we compute exactly the large devi… Show more

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Cited by 56 publications
(99 citation statements)
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“…The problem was later studied by many other authors (see e.g. [20,25,42,77]). For Brownian particles the diffusion coefficient is constant, D(ρ) = 1, and the mobility is a linear function of density, σ(ρ) = 2ρ.…”
Section: Brownian Particles With Hard-core Repulsionmentioning
confidence: 97%
“…The problem was later studied by many other authors (see e.g. [20,25,42,77]). For Brownian particles the diffusion coefficient is constant, D(ρ) = 1, and the mobility is a linear function of density, σ(ρ) = 2ρ.…”
Section: Brownian Particles With Hard-core Repulsionmentioning
confidence: 97%
“…Without any such potential, one has an SSEP with fixed (independent of space and time) hopping rates for the particles, which is an old problem [27] and has been intensively studied in the last few decades [28][29][30][31][32][33][34][35][36][37][38]. In the presence of a time-periodic potential, the hopping rates become explicit functions of time, which has not been explored much until recently [10,11,39].…”
Section: Introductionmentioning
confidence: 99%
“…In dimension d ≥ 2, tracer diffusion has been shown to remain normal, with a non trivial diffusion coefficient resulting from many-body interactions and well approximated by the Nakazato-Kitahara approach [21]. In a "single-file" geometry, where particles cannot bypass each other, the impact of EVIs is stronger and results in a subdiffusive behavior x 2 (t) ∝ t β with β = 1/2 [22][23][24][25][26][27]. In this context, determining the effect of EVIs on systems with geometrical constraints appears an important question which does not seem to have received much attention.…”
mentioning
confidence: 99%