English

Partitions, rooks, and symmetric functions in noncommuting variables

Combinatorics 2010-08-18 v1

Abstract

Let Πn\Pi_n denote the set of all set partitions of {1,2,,n}\{1,2,\ldots,n\}. We consider two subsets of Πn\Pi_n, one connected to rook theory and one associated with symmetric functions in noncommuting variables. Let \cEn\sbeΠn\cE_n\sbe\Pi_n be the subset of all partitions corresponding to an extendable rook (placement) on the upper-triangular board, \cTn1\cT_{n-1}. Given πΠm\pi\in\Pi_m and \siΠn\si\in\Pi_n, define their {\it slash product\/} to be π\si=π(\si+m)Πm+n\pi|\si=\pi\cup(\si+m)\in\Pi_{m+n} where \si+m\si+m is the partition obtained by adding mm to every element of every block of \si\si. Call τ\tau {\it atomic\/} if it can not be written as a nontrivial slash product and let \cAn\sbeΠn\cA_n\sbe\Pi_n denote the subset of atomic partitions. Atomic partitions were first defined by Bergeron, Hohlweg, Rosas, and Zabrocki during their study of NCSymNCSym, the symmetric functions in noncommuting variables. We show that, despite their very different definitions, \cEn=\cAn\cE_n=\cA_n for all n0n\ge0. Furthermore, we put an algebra structure on the formal vector space generated by all rook placements on upper triangular boards which makes it isomorphic to NCSymNCSym. We end with some remarks and an open problem.

Keywords

Cite

@article{arxiv.1008.2950,
  title  = {Partitions, rooks, and symmetric functions in noncommuting variables},
  author = {Mahir Bilen Can and Bruce E. Sagan},
  journal= {arXiv preprint arXiv:1008.2950},
  year   = {2010}
}

Comments

8 pages, 1 figure

R2 v1 2026-06-21T16:02:03.896Z