Idempotent set-theoretical solutions of the pentagon equation
Abstract
A set-theoretical solution of the pentagon equation on a non-empty set X is a function s:X× X X× X satisfying the relation s23\, s13\, s12=s12\, s23, with s12=s× \,idX, s23=idX × \, s and s13=(idX× \, τ)s12(idX× \,τ), where τ:X× X X× X is the flip map given by τ(x,y)=(y,x), for all x,y∈ X. Writing a solution as s(x,y)=(xy ,θx(y)), where θx: X X is a map, for every x∈ X, one has that X is a semigroup. In this paper, we study idempotent solutions, i.e., s2=s, by showing that the idempotents of X 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 is a monoid homomorphism.
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