Convergence to the Massive Modified Arratia Flow

Let (γn)(\gamma_n) and (n)(\ell_n) be sequences in (0,)(0,\infty), and let (Nn)(N_n) be a sequence in N+\mathbb{N}^+. For u[0,1]u\in[0,1] and t0t\geq 0, define

Zγn,nNn(u,Nnt2).Z^{N_n}_{\gamma_n,\ell_n}\left(u,\frac{N_n t}{2}\right).

Assume

Nn,n0,γnnlogNn1.N_n\to\infty,\qquad \ell_n\downarrow 0,\qquad \frac{\gamma_n\ell_n}{\log N_n}\gg 1.

Convergence conjecture. Under these assumptions,

Zγn,nNn(u,Nnt2)y(u,t)Z^{N_n}_{\gamma_n,\ell_n}\left(u,\frac{N_n t}{2}\right)\to y(u,t)

as nn\to\infty in a suitable sense, where {y(u,t):u[0,1], t[0,T]}\{y(u,t):u\in[0,1],\ t\in[0,T]\} is the Massive Modified Arratia Flow characterized by the stated axioms.

This conjecture predicts that, after clusters form in the regime of strong interaction and short interaction length, the appropriately rescaled weakly interacting diffusion system converges to a system of coalescing heavy Brownian motions represented by the Massive Modified Arratia Flow. The precise mode of convergence is left unspecified in the statement.

Sources & referencesView supporting material

Primary source

Nicolai Gerber, Rishabh S. Gvalani, Martin Hairer, Grigorios A. Pavliotis and André Schlichting, “Formation of clusters and coarsening in weakly interacting diffusions”, arXiv:2510.17629 (2026).

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