Export citation

Export citation

Choose format for download:

Download Citation

    Structure and dynamics in the low-density phase of a two-dimensional cellular automaton model of traffic flow

    Gilad Hertzberg Rabinovich, Ofer Biham, and Eytan Katzav

    Phys. Rev. E 113, 014127 – Published 21 January, 2026

    DOI: https://doi.org/10.1103/y7qy-6z9t

    Abstract

    We analyze the structure and dynamics in the low-density phase of the deterministic two-dimensional cellular automaton model of traffic flow introduced in [O. Biham, A.A. Middleton, and D. Levine, Phys. Rev. A 46, R6124(R) (1992)]. The model consists of horizontally oriented (H) cars that move to the right and vertically oriented (V) cars that move downward, on a square lattice of size L with periodic boundary conditions. Starting from a random initial state of density p, which is equally divided between the H- and V-cars, the model exhibits a phase transition at a critical density pc. For p<pc, it evolves toward a free-flowing periodic (FFP) state, while for p>pc, it evolves toward a fully jammed state or to an intermediate state of congested traffic. In the FFP states, the H- and V-cars segregate into homogeneous diagonal bands, in which they move freely without obstruction. To analyze the convergence toward the FFP states, we introduce a configuration-space distance measure D(t)=D∥(t)+D⊥(t) between the state of the system at time t and the set of FFP states. The D∥(t) term accounts for the interactions between homotypic pairs of H- (or V-) cars, while D⊥(t) accounts for the interactions between heterotypic pairs of H- and V-cars. We show that in the FFP states D(t)=0, while in all the other states D(t)>0. As the system evolves toward the FFP states, there is a separation of timescales, where D∥(t) decays very fast, while D⊥(t) decays much more slowly. Moreover, the time dependence of D⊥(t) is well fitted by an exponentially truncated power-law decay of the form D⊥(t)∼t−γexp(−t/τ⊥), where τ⊥ depends on L and p. The power-law decay suggests avalanche-like dynamics with no characteristic scale, while the exponential cutoff is imposed by the finite lattice size.

    Physics Subject Headings (PhySH)

    Authorization Required

    We need you to provide your credentials before accessing this content.

    References (Subscription Required)

    Outline

    Information

    Sign In to Your Journals Account

    Filter

    Filter

    Article Lookup

    Enter a citation