2013
DOI: 10.1103/physreve.87.062126
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One-dimensional transport of interacting particles: Currents, density profiles, phase diagrams, and symmetries

Abstract: Driven lattice gases serve as canonical models for investigating collective transport phenomena and properties of nonequilibrium steady states. Here we study one-dimensional transport with nearest-neighbor interactions both in closed bulk systems and in open channels coupled to two particle reservoirs at the ends of the channel. For the widely employed Glauber rates we derive an exact current-density relation in the bulk for unidirectional hopping. An approach based on time-dependent density functional theory … Show more

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Cited by 41 publications
(78 citation statements)
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“…This implies that in the PA the exact location of most SS phase transitions is recovered. These exact results, and as a consequence the location of most transition lines in the phase diagram, can also be obtained by using the CMF theory in [18,19] or the MCAK [12][13][14]. Let us focus on the SS phase diagram, in the limit of large lattice size N , using as parameters, in addition to q and r, the densities ρ L and ρ R .…”
mentioning
confidence: 98%
“…This implies that in the PA the exact location of most SS phase transitions is recovered. These exact results, and as a consequence the location of most transition lines in the phase diagram, can also be obtained by using the CMF theory in [18,19] or the MCAK [12][13][14]. Let us focus on the SS phase diagram, in the limit of large lattice size N , using as parameters, in addition to q and r, the densities ρ L and ρ R .…”
mentioning
confidence: 98%
“…[27][28][29][30][31][32] An elegant network representation [33] can be used to depict the transitions between the six possible states shown in Fig. 2(a).…”
mentioning
confidence: 99%
“…How theses phases change with experimentally tunable control parameters depends on details of the system reservoir couplings [40,41]. However, all possible phases can be derived from extremal current principles [36,38,41]. The arguments leading to these principles are quite general for driven diffusive systems and are valid also for driven Brownian motion.…”
Section: F Phase Transitions In Open Systemsmentioning
confidence: 99%