Mixing of fast random walks on dynamic random permutations
Luca Avena, Remco van der Hofstad, Frank den Hollander, Oliver Nagy
TL;DR
The paper investigates a fast random walk on dynamic random permutations generated by random transpositions, comparing coagulative dynamics (no fragmentation) and coagulative-fragmentative dynamics (allow fragmentation). On the scale $t\sim n$, the total variation distance to equilibrium converges to a limit process that drops once at a random drop-down time and then follows a deterministic curve linked to Erdős-Rényi giant-component sizes; the jump time distribution differs between the two dynamics. For CDP, the drop-down time converges with $\mathbb{P}(s^{\Downarrow}\le s)=\eta(s)$ and the mixing profile is $\mathcal{D}_n^{v_0}(sn) \to 1-\eta(s)\mathbb{1}_{\{}\}$, while for CFDP the drop-down time converges with $\mathbb{P}(u^{\Downarrow}\le u)=\zeta(u)$ and the mixing profile is $\mathcal{D}_n^{v_0}(un) \to 1-\zeta(u)\mathbb{1}_{\{\}}$. After the drop-down, local mixing occurs rapidly on the giant component, ensuring a single macroscopic drop in the total-variation distance and a universal decay toward equilibrium. The analysis leverages couplings between coagulative/fragementative dynamics and ER graph processes, notably cycle-free ER and Schramm’s coupling, to link permutation-cycle structure with ER giant-component behavior and to obtain precise limit laws and process-level convergence in the Skorokhod $M_1$ topology.
Abstract
We analyse the mixing profile of a random walk on a dynamic random permutation, focusing on the regime where the walk evolves much faster than the permutation. Two types of dynamics generated by random transpositions are considered: one allows for coagulation of permutation cycles only, the other allows for both coagulation and fragmentation. We show that for both types, after scaling time by the length of the permutation and letting this length tend to infinity, the total variation distance between the current distribution and the uniform distribution converges to a limit process that drops down in a single jump. This jump is similar to a one-sided cut-off, occurs after a random time whose law we identify, and goes from the value 1 to a value that is a strictly decreasing and deterministic function of the time of the jump, related to the size of the largest component in Erdős-Rényi random graphs. After the jump, the total variation distance follows this function down to 0.
