# The symmetric functions catalog

An overview of symmetric functions and related topics

2022-07-18

## Cycle index polynomials

The cycle index polynomial (Zyklenzeiger) of a group $G$ was introduced by G. Pólya in [Eq. (1,5), Pól37]. Let $G \subseteq \symS_n$ be a subgroup. The cycle index polynomial is defined in terms of the powersum symmetric functions as the average

$\cyc_G(\xvec) \coloneqq \frac{1}{|G|} \sum_{\pi \in G} \powerSum_{\type(\pi)}(\xvec).$

Let $\symS_n/G$ denote the set of let cosets of $G,$ and let $\symS_n$ act on $\setC[\symS_n/G].$ This makes $\setC[\symS_n/G]$ into an $\symS_n$-module, and its Frobenius characteristic is given by $\cyc_G(\xvec).$ In particular, $\cyc_G(\xvec)$ is Schur-positive. For more info on the cycle index polynomial, we refer to [LW19b].

Conjecture (Foulkes Conjecture, [Fou50]).

Let $X_{a,b}$ be the set of set-partitions of $\{1,2,\dotsc,ab\}$ into $a$ blocks of size $b.$ The symmetric group $S_{ab}$ act on $X_{a,b}$ in the obvious manner. Let $G_{a,b}$ be the stabilizer subgroup of some fixed element in $X_{a,b}$ under this action. Let

$\cyc_{G_{a,b}}(\xvec) = \sum_\lambda c_{\lambda,a,b}\; \schurS_\lambda(\xvec).$

Foukes conjecture states that whenever $a\leq b,$ then for all $\lambda,$ $c_{\lambda,a,b} \leq c_{\lambda,b,a}.$ This is equivalent with the statement that $\completeH_b[\completeH_a]-\completeH_a[\completeH_b]$ is Schur-positive whenever $a \leq b.$ The notation here indicates plethysm.

See also https://arxiv.org/pdf/2008.13070.pdf.

## Lyndon symmetric functions

The Lyndon symmetric functions (also known as higher Lie characters in [AHR19]) are described using the fundamental quasisymmetric functions:

$L_{\lambda}(\xvec) \coloneqq \sum_{\pi \in K_\lambda} \gessel_{n,D(w)}(\xvec)$

where $K_\lambda$ is the set of permutations in $\symS_n$ with cycle type $\lambda.$

See also [Def 1.5, AHR19] for a representation-theoretical definition.

The Lyndon symmetric functions are also covered in [p. 480, Sta01], and it was shown by Gessel–Reutenauer [Thm. 3.6, GR93], that we have

$$L_{n}(\xvec) = \frac{1}{n} \sum_{d \mid n} \mu(d)\powerSum_{d}^{n/d}, \quad L_{n^k}(\xvec) = \completeH_k[L_{n}], \quad \text{ and } \quad L_{1^{m_1}2^{m_2}\dotsb}(\xvec) = L_{1^{m_1}} L_{2^{m_2}} \dotsm.$$

These relations uniquely define the $L_{\lambda}(\xvec)$ where we write $\lambda = 1^{m_1}2^{m_2}\dotsb.$ Moreover, since $L_{n}(\xvec)$ can be shown to be Schur-positive, it follows that the Lyndon symmetric functions are also Schur positive.

Problem.

Find a combinatorial formula for the Schur expansion.

Problem (Yuval Roichman, FPSAC 2023).

Prove that for any $\lambda \vdash n$

$\sum_{k=0}^n \langle L_{\lambda}, \schurS_{k,1^{n-k} \rangle t^k$

is unimodal. This is [Conj. 7.13, AHR19].

Problem.

It is an open problem (Stanley, 2022) to find the (co)dimension of the span of the $L_\lambda,$ see 38:00 in https://www.youtube.com/watch?v=NDAzHTP3vOs.