Motivation
The two-parameter Poisson–Dirichlet distribution PD(α,θ) is a law on decreasing sequences V1≥V2≥⋯>0 with ∑nVn=1. It describes the ranked frequencies of species in Bayesian nonparametric models (the Pitman–Yor process), the ranked lengths of excursions of Bessel processes and bridges, and the ranked cycle or block sizes in random combinatorial structures. The case α=0 is Kingman's one-parameter family PD(θ), the law of the ranked frequencies in the Ewens sampling formula.
For PD(0,θ), Vershik and Shmidt ([67]) and Ignatov ([34]) found a Markov description: the residual fractions Yn=Vn/(Vn+Vn+1+⋯) form a homogeneous Markov chain, and the law is the Y1θ-tilt of a stationary chain built from independent beta(θ,1) ratios. For PD(α,0), Proposition 8 of Pitman and Yor shows that the ratios Rn=Vn+1/Vn themselves are independent beta(nα,1) variables. Theorem 38 of Pitman and Yor (Ann. Probab. 25 (1997) 855–900) unifies both descriptions for the whole two-parameter family.
Timeline. Vershik and Shmidt (1977, 1978, [66, 67]) and Ignatov (1982, [34]) described the size-ordered PD(0,θ) frequencies through the Markov chain (Yn); Ignatov showed that results of Vervaat and Watterson give the normalizing constant K0,θ=Γ(θ+1)eθγ (132). Much of this was known earlier for θ=1, the case arising in combinatorics and number theory. Perman, Pitman and Yor (1992, [51]) proved the absolute continuity of PD(α,θ) with respect to PD(α,0) (Proposition 14 here). Pitman and Yor (1997) announced the two-parameter Markov description as Theorem 15 and proved it as Theorem 38 for 0<α<1, quoting the case α=0 (Remark 40).
Setting
Fix 0<α<1 and θ>−α. The beta distribution beta(a,b) (a,b>0) has density Γ(a)Γ(b)Γ(a+b)xa−1(1−x)b−1 on (0,1). Let Y~1,Y~2,… be independent with Y~n∼beta(1−α,θ+nα), and put V~1=Y~1, V~n=(1−Y~1)⋯(1−Y~n−1)Y~n. The ranked values V1≥V2≥⋯ of (V~n) have, by Definition 1, the law PD(α,θ); Pα,θ denotes a probability under which (Vn) has this law, and Eα,θ its expectation.
From (Vn) define the ratios Rn=Vn+1/Vn (21), the residual fractions Yn=Vn/(Vn+Vn+1+⋯) (45), and Σ1=(1−V1)/V1. Conversely, from ratios define
Yn=(1+Rn+RnRn+1+⋯)−1(125).
The local time is L=limn→∞nVnα (24).
The comparison law Pα,θ∗ makes R1,R2,… independent with Rn∼beta(θ+nα,1), and Yn is then defined by (125). Constants and functions:
Kα,θ=Γ(θ+1)Γ(1−α)θ/α,Cα,θ=Γ(θ/α+1)Kα,θ,ψα(λ)=1+α∫01(1−e−λx)x−α−1dx.
Formalization targets
Goal: Theorem 38 for 0<α<1
Eα,θ[f(Y1,Y2,…)]=Kα,θEα,θ∗[Y1θf(Y1,Y2,…)](137)
for every nonnegative product measurable f; under both Pα,θ and Pα,θ∗ the sequence (Yn) is a Markov chain with the same forward transition probabilities, with density
dyn+1P(Yn+1∈dyn+1∣Yn=yn)=αyn−α−1(1−yn)nα+θ−1r(α,θ+nα−α,yn)r(α,θ+nα,yn+1)(139)
on 0<yn<1, 0<yn+1<yn/(1−yn), where r(α,θ,y)dy=Γ(θ/α+1)yθPα,θ∗(Y1∈dy)=Cα,θ−1Pα,θ(V1∈dy) (140); and the Pα,θ∗ law of Σ1 is infinitely divisible with
Eα,θ∗[e−λΣ1]=ψα(λ)−(θ/α+1)(141).
Milestones
Proposition 8 (Pα,0=Pα,0∗ on the ratios), Proposition 14 (the density Cα,θLθ/α of PD(α,θ) relative to PD(α,0)), the moments (30) of L, the representation (143) of L through the ratios, the finite-dimensional change of measure (144), its limit (145), Proposition 37 (independent ratios give a Markov chain (Yn), with co-transition density (128)), the parameter shift (146), and the conditional Laplace transform of Σ1 given X1=LV1−α.
Significance
The result. Theorem 38 reduces the size-ordered PD(α,θ) frequencies to a product of independent beta variables, up to a density Kα,θY1θ that depends on Y1 alone. Any functional of the ranked frequencies can therefore be computed under a product measure. The Markov property gives the joint density of Y1,…,Yn (Corollary 41), the laws of individual Vn (148), and the asymptotics of Yn and Σn in §7.3 of the paper. Part (iii) identifies the law of (1−V1)/V1 under Pα,θ∗, which determines the density of the largest frequency V1 under PD(α,θ).
The formalization. The result has been proved since 1997; none of it is machine-checked. The mission formalizes the paper's own route: absolute continuity (Proposition 14), the beta product structure (Proposition 8), and a limit of finite-dimensional density ratios. It produces reusable statements about real-valued Markov chains defined through conditional laws, and about changes of measure between infinite products. Note that the printed (139) omits the factor α; the formal statement includes it (see Formalization scope).
Difficulty
The finite-dimensional change of measure (144) is an exact computation, but its density (R1⋯Rn)θ degenerates as n→∞. Passing to the limit (145) requires identifying the limit of the rescaled densities nθ/α(R1⋯Rn)θ with Lθ/αY1−θ, and an almost sure limit of densities does not by itself give the identity of expectations. A second obstacle is that the Markov property of (Yn) under Pα,θ does not follow from any independence under Pα,θ itself; it is transported from Pα,θ∗ through a density that is a function of Y1 only, and the transported kernels must be shown to be the same. Part (iii) needs the Laplace transform of 1/V1 conditioned on X1, which comes from the Poisson structure of PD(α,0).
Formalization scope
Sequences are ℕ → ℝ, 0-based: V ω k is Vk+1, Yseq v k and YofR r k are Yk+1. "(Vn) has PD(α,θ) law" (HasPD) means that measures of preimages of measurable sets agree with those of the ranked stick-breaking map under an independent beta product (IsStickLaw); ranking counts exceedances with Set.encard. Pα,θ∗ is any probability measure on ℕ → ℝ with independent coordinates of the stated beta laws (IsStarLaw); it is defined directly as a product, never through Pα,θ. The local time L is a random variable given with its defining almost sure limit (24). A Markov chain with forward kernels κn (IsMarkovWith) is stated through the defining identity E[g(Y1..Yn)h(Yn+1)]=E[g(Y1..Yn)∫hdκn(Yn)]; Theorem 38 (ii) asks for one family of Markov kernels serving both laws. The function r of (140) is a hypothesis: any function giving the density of Y1 under each Pα,θ+kα∗.
Committed deviations: the goal is the case 0<α<1, the case the paper proves (the case α=0 is quoted from [67], [34]); (139) carries the factor α that Bayes' rule from (128), (146) and the beta densities produces, and that Corollary 41's αn−1 confirms; (30) omits its middle expression CpE(Σ−αp). Every expectation of a nonnegative quantity is a lower Lebesgue integral, so no identity can hold through the junk value of a non-integrable Bochner integral; no law is written as Measure.map of a possibly non-measurable function; no limit is taken with limUnder; and the parameter range 0<α<1, θ>−α is a hypothesis of every statement that uses it.
Contributions welcome: the product-measure and beta-density computations behind (144) and (146), the limit passage (145), the Markov property of functions of independent sequences (Proposition 37), and the transfer of a Markov property through a density depending on the first coordinate.
Selected references
- J. Pitman and M. Yor, The two-parameter Poisson–Dirichlet distribution derived from a stable subordinator, Ann. Probab. 25(2) (1997), 855–900. https://doi.org/10.1214/aop/1024404422
- A. M. Vershik and A. A. Shmidt, Limit measures arising in the theory of groups, I, Theory Probab. Appl. 22 (1977), 79–85; II, Theory Probab. Appl. 23 (1978), 36–49 (references [66], [67] of the paper; no link verified).
- Ts. Ignatov, On a constant arising in the theory of symmetric groups and on Poisson–Dirichlet measures, Theory Probab. Appl. 27 (1982), 136–147 (reference [34] of the paper; no link verified).
- M. Perman, J. Pitman and M. Yor, Size-biased sampling of Poisson point processes and excursions, Probab. Theory Related Fields 92 (1992), 21–39. https://doi.org/10.1007/BF01205234