2015
DOI: 10.1103/physrevlett.115.240602
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Anomalous Magnetotransport in Disordered Structures: Classical Edge-State Percolation

Abstract: By event-driven molecular dynamics simulations we investigate magnetotransport in a two-dimensional model with randomly distributed scatterers close to the field-induced localization transition. This transition is generated by percolating skipping orbits along the edges of obstacle clusters. The dynamic exponents differ significantly from those of the conventional transport problem on percolating systems, thus establishing a new dynamic universality class. This difference is tentatively attributed to a weak-li… Show more

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Cited by 28 publications
(40 citation statements)
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References 63 publications
(109 reference statements)
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“…gravitational) force [21]. It also serves as a reference to characterize the non-equilibrium behavior of these chiral particles exposed to spatially heterogeneous media [52,53]. Similarly, it might be a useful input to establish sorting mechanisms of microswimmers according to their (chiral) transport properties [34,54].…”
Section: Discussionmentioning
confidence: 99%
“…gravitational) force [21]. It also serves as a reference to characterize the non-equilibrium behavior of these chiral particles exposed to spatially heterogeneous media [52,53]. Similarly, it might be a useful input to establish sorting mechanisms of microswimmers according to their (chiral) transport properties [34,54].…”
Section: Discussionmentioning
confidence: 99%
“…A heterogeneous environment can be realized in different ways, both in experiments and theory, e.g., by regular or irregular patterns of obstacles [20][21][22][23][24][25][26][27][28][29][30][31][32], mazes [33], arrays of funnels [16,[34][35][36][37][38], pinning substrates [39], or patterned light fields, which control the velocity of the microswimmer [40,41]. For a review see [4,42].…”
Section: Introductionmentioning
confidence: 99%
“…This has been rationalized [54,55] by an underlying percolation transition of disks made of obstacles and 'halos' thus associating an effective radius σ + R to each obstacle. Last, at densities n * > n * c a localized state emerges since the void space between the obstacles ceases to percolate, such that the microswimmers are trapped in separated pockets of void space, resulting in no long-range transport.…”
Section: Model and Methodsmentioning
confidence: 99%