Density decay and growth of correlations in the Game of Life

We study the Game of Life as a statistical system on an $L\times L$ square lattice with periodic boundary conditions. Starting from a random initial configuration of density $ρ_{\rm in}=0.3$ we investigate the relaxation of the density as well as the growth with time of spatial correlations. The asymptotic density relaxation is exponential with a characteristic time $τ_L$ whose system size dependence follows a power law $τ_L\propto L^z$ with $z=1.66\pm 0.05$ before saturating at large system sizes to a constant $τ_\infty$. The correlation growth is characterized by a time dependent correlation length $ξ_t$ that follows a power law $ξ_t\propto t^{1/z^\prime}$ with $z^\prime$ close to $z$ before saturating at large times to a constant $ξ_\infty$. We discuss the difficulty of determining the correlation length $ξ_\infty$ in the final "quiescent" state of the system. The decay time $t_{\rm q}$ towards the quiescent state is a random variable, we present simulational evidence as well as a heuristic argument indicating that for large $L$ its distribution peaks at a value $t_{\rm q}^*(L) \simeq 2τ_\infty\log L$.