Self-absorption of Hankel systems on monoids --a seemingly universal property

TL;DR

This paper investigates the self-absorption property of Hankel systems associated with cancellative monoids and extends the concept to generalized systems, with applications in Fourier analysis and operator theory.

Contribution

It introduces a new algebraic condition ensuring self-absorption for Hankel systems of monoids and generalizes this property to broader classes of maps and systems.

Findings

Self-absorption holds for all group-embeddable monoids.

Hereditary self-absorption for generalized Hankel systems.

Applications to Fourier multipliers and operator norms.

Abstract

Given any cancellative monoid $\mathcal{M}$, we study the Hankel system determined by its multiplication table. We prove that the Hankel system admits self-absorption property provided that the monoid $\mathcal{M}$ has the local algebraic structure: \[ \big(ax = by, cx=dy, az=bw \,\, \text{in $\mathcal{M}$}\big)\Longrightarrow \big(cz=dw \,\, \text{in $\mathcal{M}$}\big). \] Our result holds for all group-embeddable monoids and goes beyond. In particular, it works for all cancellative Abelian monoids and most common non-Abelian cancellative monoids such as $$ \mathrm{SL}_d(\mathbb{N}): = \big\{[a_{ij}]_{1\le i,j\le d}\in \mathrm{SL}_d(\mathbb{Z})\big| a_{ij} \in \mathbb{N}\big\}. $$ The Hankel system determined by the multiplication table of a monoid is further generalized to that determined by level sets of any abstract two-variable map. We introduce an algebraic notion of lunar maps and establish a stronger hereditary self-absorption property for the corresponding generalized Hankel systems. As a consequence, we prove the self-absorption property for arbitrary spatial compression of the regular representation system $\{\lambda_G(g)\}_{g\in G}$ of any discrete group $G$, as well as the Hankel system $\{\Gamma_\ell^\Phi\}$ determined by the level sets of any rational map of the form $\Phi(x,y)=a x^m + b y^n$ with $a,b,m,n\in \mathbb{Z}^*$: \[ \Gamma_\ell^{\Phi}(x, y)= \mathbf{1}(a x^m + b y^n= \ell), \quad x, y\in \mathbb{N}^*, \, \ell\in \Phi (\mathbb{N}^*\times \mathbb{N}^*). \] The self-absorption property is applied to the study of completely bounded Fourier multipliers between Hardy spaces. Further applications are: i) exact complete bounded norm of the Carleman embedding in any dimension; ii) mixed Fourier-Schur multiplier inequalities with critical exponent $4/3$; iii) failure of hyper-complete-contractivity for the Poisson semigroup.