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About the Cramér Large Deviation Property for Bell Polynomials

Sophia Li, Shannon Starr

Source record

Source: arXiv

Published: Sep 5, 2026

arXiv: 2609.06281

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Source abstract

If w=(w1,w2,)\boldsymbol{w} = (w_1,w_2,\dots) is a sequence in N={1,2,}\mathbb{N}=\{1,2,\dots\}, the partial Bell polynomials based on w\boldsymbol{w} are Bn,kB_{n,k} for kNk \in \mathbb{N} and n{k,k+1,}n\in\{k,k+1,\dots\}. Let F(z)=n=1(wn/n!)znF(z) = \sum_{n=1}^{\infty} (w_n/n!)z^n be the exponential generating function for w\boldsymbol{w}, and assume the radius of convegence is positive R>0R>0. Then F(z)k=n=k(k!/n!)znBn,kF(z)^k = \sum_{n=k}^{\infty} (k!/n!) z^n B_{n,k} for z<R|z|<R. Alternatively, defining Qk,n=(k!/n!)Bn,kQ_{k,n} = (k!/n!)B_{n,k}, we have Q1,n=wn/n!Q_{1,n} = w_n/n!, and Qk+1,n=m=1nkQ1,mQk,nmQ_{k+1,n}=\sum_{m=1}^{n-k} Q_{1,m} Q_{k,n-m} for k1k\geq 1. Let us say that the Cramér-type large deviation property holds if limnk/nκ1nln(Qk,n)=G(κ), \lim_{\substack{n \to \infty\\ k/n \to κ}} \frac{1}{n}\, \ln\left(Q_{k,n}\right)\, =\, \mathcal{G}(κ)\, , for every κ(0,1)κ\in (0,1), where G(κ)=infr(0,R)(κln(F(r))ln(r))\mathcal{G}(κ)=\inf_{r \in (0,R)} (κ\ln(F(r))-\ln(r)). The (Hardy-Ramanujan) Erdös induction argument suggests this should generally be true as long as two technical conditions are true: one an initial step, and the other a condition for small densities κκ.

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