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Stirling operators in spatial combinatorics

Published 1 Jul 2020 in math.CO, math-ph, math.FA, math.MP, and math.PR | (2007.01175v6)

Abstract: We define and study a spatial (infinite-dimensional) counterpart of Stirling numbers. In classical combinatorics, the Pochhammer symbol $(m)n$ can be extended from a natural number $m\in\mathbb N$ to the falling factorials $(z)_n=z(z-1)\dotsm (z-n+1)$ of an argument $z$ from $\mathbb F=\mathbb R\text{ or }\mathbb C$, and Stirling numbers of the first and second kinds are the coefficients of the expansions of $(z)_n$ through $zk$, $k\leq n$ and vice versa. When taking into account spatial positions of elements in a locally compact Polish space $X$, we replace $\mathbb N$ by the space of configurations -- discrete Radon measures $\gamma=\sum_i\delta{x_i}$ on $X$, where $\delta_{x_i}$ is the Dirac measure with mass at $x_i$.The spatial falling factorials $(\gamma)n:=\sum{i_1}\sum_{i_2\ne i_1}\dotsm\sum_{i_n\ne i_1,\dots, i_n\ne i_{n-1}}\delta_{(x_{i_1},x_{i_2},\dots,x_{i_n})}$ can be naturally extended to mappings $M{(1)}(X)\ni\omega\mapsto (\omega)n\in M{(n)}(X)$, where $M{(n)}(X)$ denotes the space of $\mathbb F$-valued, symmetric (for $n\ge2$) Radon measures on $Xn$. There is a natural duality between $M{(n)}(X)$ and the space $\mathcal {CF}{(n)}(X)$ of $\mathbb F$-valued, symmetric continuous functions on $Xn$ with compact support. The Stirling operators of the first and second kind, $\mathbf{s}(n,k)$ and $\mathbf{S}(n,k)$, are linear operators, acting between spaces $\mathcal {CF}{(n)}(X)$ and $\mathcal {CF}{(k)}(X)$ such that their dual operators, acting from $M{(k)}(X)$ into $M{(n)}(X)$, satisfy $(\omega)_n=\sum{k=1}n\mathbf{s}(n,k)*\omega{\otimes k}$ and $\omega{\otimes n}=\sum_{k=1}n\mathbf{S}(n,k)*(\omega)_k$, respectively. We derive combinatorial properties of the Stirling operators, present their connections with a generalization of the Poisson point process and with the Wick ordering under the canonical commutation relations.

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