Alphabeta Math
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Joint convergence in distribution and the normalized cycle-character observables

Definition

Fix an integer N≥2. For n≥1 and 2≤k≤N define the real random variable ηk(n)(λ):=pk#(λ)k nk/2,λ⊢n, on the finite probability space (Yn,Pn) of The Plancherel measure on the partitions of n, whose weights are nonnegative and sum to one by The Plancherel weights sum to one, where pk# is the shifted character observable of Shifted character observables pρ# and profile moments p~k; since pk# is a real function on Yn, each ηk(n) is a real random variable on the finite space Yn. Let η(n):=(η2(n),…,ηN(n)):Yn→RN−1 be the corresponding RN−1-valued random element, with law the pushforward of Pn (Law or distribution of a random element).

Joint convergence in distribution of such vectors means convergence in distribution of random elements in the sense of Convergence in distribution of random elements: if η(n) has law μn and η has law μ on RN−1, then η(n)⟹η means μn⇒μ weakly, that is, ∫f dμn→∫f dμ for every bounded continuous real function f on RN−1.

The standard Gaussian target law is NN−1(0,IN−1) (Multivariate normal law, including singular covariance), the law of a vector with independent standard normal coordinates; under AC this multi-dimensional law exists and is available in the library. For independent standard Gaussian random variables ξk, 2≤k≤N, this target is the law of (ξ2,…,ξN). The unnormalized observables pk#/nk/2 instead have the target coordinates ζk:=k ξk, independent centered Gaussians of variances k; the normalization ηk(n)=pk#/(k nk/2) is chosen so that this is the limit asserted in Kerov's central limit theorem for normalized cycle characters. No convergence is asserted in this definition, and no choice principle is used beyond the existence of the target law.

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