2020-08-11
Lah symmetric functions
The Lah symmetric functions were introduced in [PS19b]. They are indexed by two integers, $n \geq k \geq 1.$ The combinatorial description is as follows.
We first need the notion of an increasing ordered tree on vertex set $[n].$ Each node has label smaller than its children (so vertex labeled $1$ is a root), and the children are ordered linearly. The number of such trees on $n$ nodes are given by $1,$ $1,$ $3,$ $15,$ $105,\dotsc,$ see A001147.
An unordered forest on increasing ordered trees is a forest on vertex set $[n],$ where each component is an increasing ordered tree. The number of such forests on $n$ vertices with $k$ trees is given by A001497:
$n \backslash k$ | $\textbf{1}$ | $\textbf{2}$ | $\textbf{3}$ | $\textbf{4}$ | $\textbf{5}$ | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
$\textbf{1}$ | $1$ | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
$\textbf{2}$ | $1$ | $1$ | |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
$\textbf{3}$ | $3$ | $3$ | $1$ | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
$\textbf{4}$ | $15$ | $15$ | $6$ | $1$ | |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
$\textbf{5}$ | $105$ | $105$ | $45$ | $10$ | $1$ | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
The Lah symmetric function is then defined as
\[ \lah_{n,k}(\xvec) \coloneqq \sum_{F \in \mathrm{Forests}(n,k)} \prod_{j=1}^n \elementaryE_{c(j)}(\xvec) \]where $c(j)$ is the number of children of vertex $j,$ and the sum is taken over all unordered forest on increasing ordered trees, with $n$ vertices and exactly $k$ trees. By definition, the $\lah_{n,k}(\xvec)$ are positive in the elementary symmetric function basis.
Note: the $\lah_{n,k}(\xvec)$ is denoted $L^{(\infty)+}_{n,k}(X)$ and $L^{(\infty)-}_{n,k}(X) = \omega \lah_{n,k}(\xvec)$ in [PS19b].
We have that
\begin{align*} \lah_{4,1} &= 6 \elementaryE_3 + 8 \elementaryE_{21} + \elementaryE_{3} = \monomial_{3} + 11\monomial_{21}+36\monomial_{111}, \\ \lah_{4,2} &= 8 \elementaryE_2 + 7 \elementaryE_{11} = 7\monomial_{2} + 22\monomial_{11} \\ \lah_{4,3} &= 6 \elementaryE_{1}= 6\monomial_{1} \\ \lah_{4,4} &= 1. \end{align*}References
- [PS19b] Mathias Pétréolle and Alan D. Sokal. Lattice paths and branched continued fractions. II. multivariate LAH polynomials and LAH symmetric functions. arXiv e-prints, 2019.