Anomalous current fluctuations and mobility-driven clustering
arXiv:2506.00949 · doi:10.1088/1742-5468/adfa77
Abstract
We study steady-state current fluctuations in hardcore lattice gases on a ring of sites, where particles perform symmetric, {\it extended-ranged} hopping. The hop length is a random variable depending on a length scale (hopping range) and the inter-particle gap. The systems have mass-conserving dynamics with global density fixed, but violate detailed balance. We consider two analytically tractable cases: (i) (finite-ranged) and (ii) (infinite-ranged); in the latter, the system undergoes a clustering or condensation transition below a critical density . In the steady state, we compute, exactly within a closure scheme, the variance of the cumulative (time-integrated) current across a bond over a time interval . We show that for , the scaled variance of the time-integrated bond current, or equivalently, the mobility diverges at . That is, near criticality, the mobility has a simple-pole singularity, thus providing a dynamical characterization of the condensation transition, previously observed in a related mass aggregation model by Majumdar et al.\ [{\it Phys.\ Rev.\ Lett.\ {\bf 81}, 3691 (1998)}]. At the critical point , the variance has a scaling form with and the dynamical exponent . Thus, near criticality, the mobility {\it diverges} while the diffusion coefficient remains {\it finite}, {\it unlike} in equilibrium systems with short-ranged hopping, where diffusion coefficient usually {\it vanishes} and mobility remains finite.
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