On the norm of the $q$-circular operator
Abstract
The -commutation relations, formulated in the setting of the -Fock space of Bo\.zjeko and Speicher, interpolate between the classical commutation relations (CCR) and the classical anti-commutation relations (CAR) defined on the classical bosonic and fermionic Fock spaces, respectively. Interpreting the -Fock space as an algebra of "random variables" exhibiting a specific commutativity structure, one can construct the so-called -semicircular and -circular operators acting as -deformations of the classical Gaussian and complex Gaussian random variables, respectively. While the -semicircular operator is generally well understood, many basic properties of the -circular operator (in particular, a tractable expression for its norm) remain elusive. Inspired by the combinatorial approach to free probability, we revist the combinatorial formulations of these operators. We point out that a finite alternating-sum expression for -norm of the -semicircular is available via generating functions of chord-crossing diagrams developed by Touchard in the 1950s and distilled by Riordan in 1974. Extending these norms as a function in onto the complex unit ball and taking the limit, we recover the familiar expression for the norm of the -semicircular and show that the convergence is uniform on the compact subsets of the unit ball. In contrast, the -norms of the -circular are encoded by chord-crossing diagrams that are parity-reversing, which have not yet been characterized in the combinatorial literature. We derive certain combinatorial properties of these objects, including closed-form expressions for the number of such diagrams of any size with up to eleven crossings. These properties enable us to conclude that the -norms of the -circular operator are significantly less well behaved than those of the -semicircular operator.
Keywords
Cite
@article{arxiv.1102.0748,
title = {On the norm of the $q$-circular operator},
author = {Natasha Blitvić},
journal= {arXiv preprint arXiv:1102.0748},
year = {2011}
}