Coalescents With Multiple Collisions 1: A Coalescent on Partitions of ℕ With k-Fold Merger Rates λ_{b,k} Exists Iff λ_{b,k} = ∫ x^{k−2}(1−x)^{b−k} Λ(dx)Research Paper
Motivation
A coalescent models a collection of ancestral lineages merging as time runs backward. If every event joins exactly two lineages, a single pairwise merger rate describes the finite system. Pitman’s 1999 paper asks which rates permit an event to join any number of blocks, while still giving one process on partitions of all positive integers. This matters when a sample of any finite size must be a restriction of the same population model: specifying a chain separately at every sample size is insufficient unless the chains agree when labels are removed. The paper supplies an exact answer in terms of a finite measure on the unit interval. See Pitman (1999), Theorem 1 and §3.1.
Setting
Let be the partitions of and the partitions of the positive integers. A partition records which labels belong to the same block. The map restricts a partition to . A partition refines when every block of is contained in a block of . Thus blocks can merge as time grows, but never split.
A -valued process is a coalescent here when its paths refine with time and each finite restriction has right-continuous step-function paths. For a partition of with blocks, each unordered choice of blocks, , merges into one block at rate . Different choices are different possible transitions, each with that rate; the rate is not multiplied by the number of choices. The finite chain’s generator records these transition rates, with each diagonal entry the negative sum of the other entries in its row. Its transition matrix after time is .
An array is consistent when, for every and every initial partition of , restricting the -label chain to gives the same process law as the -label chain started at the restricted partition. A finite nonnegative Borel measure on supplies a rate array through an integral. The point mass at zero is included: because for natural powers, it gives pairwise mergers while higher-order merger rates vanish. These definitions follow Pitman (1999), pp. 1871–1872 and Lemma 18.
Formalization targets
Characterization of admissible rates
The goal is the existence-and-rates part of Theorem 1. For every nonnegative array , a coalescent with these finite-chain merger rates exists from every if and only if there is a finite nonnegative measure on such that
The statement asks for one measure representing every rate in the infinite array, and a process from every initial partition. It fixes neither a particular measure nor a sample size. This is Theorem 1, equation (1).
Supporting claims
The milestone list follows §3.1: adjacent-size restrictions suffice to check consistency; consistency is equivalent to
and the nonnegative normalized array relation
is equivalent to a representation for . The final milestone states the uniqueness as well as the existence of the representing measure: equation (1) is a bijection between consistent arrays and finite measures. These are the claims in Lemma 18 and its proof, p. 1882.
Significance
The characterization turns an infinite family of nonnegative rates into one finite measure, and says exactly when finite chains at different sample sizes can be restrictions of a common partition process. The bijection also makes the measure identifiable from the rates. Without consistency, a chain specified at one size can change its law when an unobserved extra label is added; there would be no single process on with those restrictions.
Pitman proved these results in 1999. The mission concerns machine-checking their statements and, eventually, their proofs. The current Lean items are open theorems with compiled statements; they do not yet have machine-checked proofs. The reusable part of a complete development would include finite partition generators, restriction of continuous-time Markov chains, and the moment representation for normalized nonnegative arrays. These tools also apply to other consistent families of random combinatorial structures.
Difficulty
Checking that each defines a finite-state chain does not by itself construct a process on partitions of all integers. Deleting one label can change which apparent merger occurs in the smaller chain, so the rates must satisfy a precise identity across adjacent sizes. Even once those identities hold, the conclusion requires one joint law whose finite restrictions agree for all sizes and times, with right-continuous paths. The representation step must recover a genuine finite measure, including possible mass at zero, and must prove uniqueness; a mere numerical fit for finitely many entries cannot establish the theorem.
Formalization scope
The Lean partition type is Setoid (Fin n) at finite size and a type synonym of Setoid ℕ at infinite size. The paper’s positive labels are shifted to zero-based labels, preserving their order. The measurable structure on infinite partitions is generated by pairwise equivalence coordinates, equivalently by finite restrictions; finite partition spaces use the discrete measurable structure. The process path predicate requires refinement at every pair of ordered times and right continuity of every finite restriction. Finite-chain laws are specified at all finite collections of times through , so a process cannot qualify merely by having the right initial state or a single marginal.
The measure is represented on with zero mass outside [0,1]x^0=1x=02\le k\le b$, and the zero measure is allowed. The Fin 0 restriction is an additional tautological boundary case introduced by Lean’s natural numbers. The process sample space is a small Lean type, and the law is a probability measure on it.
Only the characterization sentence of Theorem 1 is targeted. Its later assertions about the strong Markov property, Feller semigroup, Skorohod path-space law, and weak continuity of the law map are outside this mission. Contributions toward those properties would need further path-space infrastructure. The formalized foundations and milestones can also support the paper’s Poisson construction and its later results, but those are separate targets.
Selected references
- Jim Pitman, Coalescents with multiple collisions, Annals of Probability 27(4), 1870–1902, 1999. DOI: 10.1214/aop/1022874819.