We study the late-time coarsening dynamics of a scalar coherence field C (x, t) ∈ 0, 1 governed by a bistable Allen–Cahn / Wright–Fisher reaction–diffusion equation in a spatially flat FRW background. This work does not dispute the Boyanovsky–de Vega scaling result for symmetry breaking in FRW cosmologies; it identifies a distinct late-time dissipative regime in which the observables, assumptions, and effective dynamics differ from those of the large-N quantum-field calculation. Through deterministic numerical integration on a periodic cubic lattice, we establish that the characteristic comoving length scale obeys the calibrated law ℓ² (t) = b + A·DC·∫dt'/a² (t'), with a single effective prefactor A = 7. 67 ± 0. 20 consistent across four independent backgrounds (Minkowski, radiation, matter, de Sitter) with R² ≥ 0. 996 in the pre-saturation window. The naïve dimensional estimate A = 2 is excluded; the exact prefactor is a measured property of the factorized Wright–Fisher kernel, not a universal constant. In de Sitter the accumulated comoving diffusion time saturates to 1/ (2H), and we confirm numerically the corresponding double-freezing of the coarsening scale. The bistable front velocity supports the Aronson–Weinberger prediction in sign across all three FRW backgrounds and quantitatively in the best-resolved de Sitter case. A finite-noise robustness check (σ=0. 1, radiation) shows the law survives in functional form with the prefactor renormalized downward ~20%. We delimit the domain of validity of this late-time dissipative description relative to the large-N quantum regime and identify the transition between the two (Regime II) as an explicit open problem.
Arturo Cerezo (Sat,) studied this question.