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arxiv: 2605.16244 · v1 · pith:OOWYULWNnew · submitted 2026-05-15 · 🧮 math.PR · math.CO

Burnside process on parking functions and Dyck paths

Pith reviewed 2026-05-19 18:21 UTC · model grok-4.3

classification 🧮 math.PR math.CO
keywords Burnside processparking functionsDyck pathsMarkov chain mixinguniform samplingCatalan structurestriangulationsgroup actions
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The pith

The Burnside process on parking functions and labeled Dyck paths mixes in O(n log n) steps and yields uniform sampling algorithms.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper studies a Markov chain called the Burnside process that arises from a finite group acting on a set and projects to uniform distribution over the orbits. It applies the construction in two cases: parking functions of length n with the symmetric group permuting coordinates, and labeled Dyck paths of length 2n with the symmetric group permuting labels. The central result establishes that both chains reach stationarity in at most O(n log n) steps. This bound supplies practical algorithms for sampling an increasing parking function or a Dyck path approximately uniformly at random. The same technique also produces approximate uniform samples of triangulations of an (n+2)-gon.

Core claim

The Burnside processes defined on the set of parking functions of length n under the action of S_n by coordinate permutation and on the set of labeled Dyck paths of length 2n under the action of S_n by label permutation both mix rapidly, with mixing times bounded above by O(n log n). This establishes new Markov-chain algorithms that output an increasing parking function or a Dyck path approximately uniformly at random, and the same processes can be used to sample triangulations of an (n+2)-gon approximately uniformly at random.

What carries the argument

The Burnside process, a Markov chain on the underlying set whose transitions are chosen so that the projected chain on orbits has uniform stationary distribution.

Load-bearing premise

The specific group actions of S_n on parking functions by coordinate permutation and on Dyck paths by label permutation allow the Burnside process to maintain uniform stationary distribution on orbits and to mix rapidly under the given transition rules.

What would settle it

A direct computation or simulation for some large n showing that the total-variation distance to the uniform distribution on orbits stays larger than 1/4 after more than C n log n steps for any fixed constant C would falsify the claimed mixing-time upper bound.

Figures

Figures reproduced from arXiv: 2605.16244 by Ivan Z. Feng, J. E. Paguyo.

Figure 1
Figure 1. Figure 1: (a) The Dyck path (given by the sequence N2E E NE N2E E) corresponding to the increasing parking function u = (1, 1, 3, 4, 4). (b) The labeled Dyck path corresponding to the parking function x = (4, 1, 3, 4, 1). Let X = LDn and let G = Sn act on LDn as follows. Given σ ∈ Sn, replace the label i by σ(i), and then rearrange the labels along each vertical run so that they are in increasing order. See [PITH_F… view at source ↗
Figure 2
Figure 2. Figure 2: Example of the group action of S5 on labeled Dyck paths LD5. Here σ = (1 5 3)(2 4). Let Gx be the stabilizer of x ∈ LDn and let Xσ be the fixed set of σ under this group action of Sn on LDn. The Burnside process on labeled Dyck paths (henceforth, the Burnside process on LDn), is a Markov chain whose transition between states x, y ∈ LDn is described by the following two-step procedure: • From x ∈ LDn, pick … view at source ↗
read the original abstract

Let $G$ be a finite group acting on a finite set $X$. This group action splits $X$ into disjoint orbits. The Burnside process is a Markov chain on $X$ which has a uniform stationary distribution when the chain is projected to orbits. We initiate the study of the Burnside process on Catalan structures. We consider two special cases: the first where the state space is the set of parking functions of length $n$ and $G = S_n$ is the symmetric group on $[n]$, such that $G$ acts by permuting coordinates, and the second where the state space is the set of labeled Dyck paths of length $2n$ and $G = S_n$ acts by permuting labels. The resulting Burnside processes give novel algorithms for sampling, respectively, an increasing parking function and a Dyck path approximately uniformly at random. Our main result shows that both processes are rapidly mixing, with mixing times upper bounded by $O(n \log n)$. As an application, we show how our Burnside process can be used to sample triangulations of an $(n+2)$-gon approximately uniformly at random.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

0 major / 3 minor

Summary. The manuscript introduces the Burnside process on two families of Catalan structures: parking functions of length n under the coordinate-permutation action of S_n, and labeled Dyck paths of length 2n under the label-permutation action of S_n. It shows that the resulting Markov chains have uniform stationary distribution on orbits and proves, via explicit coupling arguments, that both chains are rapidly mixing with mixing-time upper bound O(n log n). The work concludes with an application to approximate uniform sampling of triangulations of an (n+2)-gon via the standard Dyck-path bijection.

Significance. If the stated mixing-time bounds hold, the paper supplies concrete, efficient sampling algorithms for increasing parking functions and for Dyck paths, objects central to enumerative combinatorics. Credit is due for the explicit coupling constructions that rely only on standard combinatorial facts (increasing orbit representatives, recursive structure of Dyck paths) rather than black-box theorems, and for the direct derivation of the triangulation-sampling application.

minor comments (3)
  1. [§2] §2, definition of the Burnside process: the transition probabilities are written in terms of fixed-point counts; a short sentence recalling that the chain is well-defined on the full set X (not only on orbits) would aid readers unfamiliar with the general construction.
  2. [Theorem 3.4] Theorem 3.4 (parking-function mixing time): the coupling argument tracks coordinate coalescence but does not explicitly bound the probability that a given coordinate has not yet been hit after t steps; adding this one-line estimate would make the O(n log n) derivation fully self-contained.
  3. [Figure 1] Figure 1 (Dyck-path example): the labels on the path are printed in a font size that is difficult to read at standard journal resolution; increasing the font or adding a magnified inset would improve clarity.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for their positive summary, recognition of the significance of the mixing-time results, and recommendation for minor revision. No specific major comments were raised in the report, so we have no points to address individually at this stage. We will incorporate any minor editorial suggestions in the revised manuscript.

Circularity Check

0 steps flagged

No significant circularity; derivation self-contained

full rationale

The paper applies the general Burnside process (defined via group actions on orbits) to parking functions under S_n coordinate permutation and to labeled Dyck paths under label permutation. Uniformity on orbits follows immediately from the standard Burnside process construction without redefinition. The O(n log n) mixing-time upper bounds are derived via separate explicit coupling arguments that track coordinate/label coalescence, using only standard combinatorial facts (increasing orbit representatives, Dyck path recursion) that are independently verifiable. No fitted parameters are renamed as predictions, no self-citation chain carries the central claim, and the triangulation-sampling application rests on the pre-existing Dyck-path bijection. The derivation chain is therefore independent of its inputs and contains no circular reductions.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The paper relies on the general definition of the Burnside process and its uniform stationary distribution on orbits under group actions, with no free parameters, invented entities, or additional axioms mentioned in the abstract.

axioms (1)
  • domain assumption The Burnside process has a uniform stationary distribution when the chain is projected to orbits.
    Stated as the general property of the Burnside process in the setup before the two special cases.

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Reference graph

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