English

Idempotent set-theoretical solutions of the pentagon equation

Quantum Algebra 2023-08-22 v2

Abstract

A set-theoretical solution of the pentagon equation on a non-empty set XX is a function s:X×XX×Xs:X\times X\to X\times X satisfying the relation s23s13s12=s12s23s_{23}\, s_{13}\, s_{12}=s_{12}\, s_{23}, with s12=s×idXs_{12}=s\times \,id_X, s23=idX×ss_{23}=id_X \times \, s and s13=(idX×τ)s12(idX×τ)s_{13}=(id_X\times \, \tau)s_{12}(id_X\times \,\tau), where τ:X×XX×X\tau:X\times X\to X\times X is the flip map given by τ(x,y)=(y,x)\tau(x,y)=(y,x), for all x,yXx,y\in X. Writing a solution as s(x,y)=(xy,θx(y))s(x,y)=(xy ,\theta_x(y)), where θx:XX\theta_x: X \to X is a map, for every xXx\in X, one has that XX is a semigroup. In this paper, we study idempotent solutions, i.e., s2=ss^2=s, by showing that the idempotents of XX have a key role in such an investigation. In particular, we describe all such solutions on monoids having central idempotents. Moreover, we focus on idempotent solutions defined on monoids for which the map θ1\theta_1 is a monoid homomorphism.

Cite

@article{arxiv.2301.01643,
  title  = {Idempotent set-theoretical solutions of the pentagon equation},
  author = {Marzia Mazzotta},
  journal= {arXiv preprint arXiv:2301.01643},
  year   = {2023}
}