Joint spectrum and infinite dihedral group

TL;DR

This paper computes the joint spectrum of specific elements in the group $C^*$-algebra of the infinite dihedral group, revealing self-similar structures and linking spectral properties to group representations and dynamics.

Contribution

It provides explicit formulas for the joint spectrum and Fuglede-Kadison determinant for the infinite dihedral group, and demonstrates the self-similar nature of its $C^*$-algebra.

Findings

Joint spectrum computed for $(1,a,t)$ in $D_{ extinfty}$

Fuglede-Kadison determinant formula derived

Self-similar structure of $C^*(D_{ extinfty})$ revealed

Abstract

For a tuple $A=(A_1,\ A_2,\ ...,\ A_n)$ of elements in a unital Banach algebra ${\mathcal B}$, its {\em projective joint spectrum} $P(A)$ is the collection of $z\in {\mathbb C}^n$ such that the multiparameter pencil $A(z)=z_1A_1+z_2A_2+\cdots +z_nA_n$ is not invertible. If ${\mathcal B}$ is the group $C^*$-algebra for a discrete group $G$ generated by $A_1,\ A_2,\ ...,\ A_n$ with respect to a representation $\rho$, then $P(A)$ is an invariant of (weak) equivalence for $\rho$. This paper computes the joint spectrum of $(1,\ a,\ t)$ for the infinite dihedral group $D_{\infty}=<a,\ t\ |\ a^2=t^2=1>$ with respect to the left regular representation $\lambda_D$, and gives an in-depth analysis on its properties. A formula for the Fuglede-Kadison determinant of the pencil $R(z)=1+z_1a+z_2t$ is obtained, and it is used to compute the first singular homology group of the joint resolvent set $P^c(R)$. The joint spectrum gives new insight into some earlier studies on groups of intermediate growth, through which the corresponding joint spectrum of $(1,\ a,\ t)$ with respect to the Koopman representation $\rho$ (constructed through a self-similar action of $D_{\infty}$ on a binary tree) can be computed. It turns out that the joint spectra with respect to the two representations coincide. Interestingly, this fact leads to a self-similar realization of the group $C^*$-algebra $C^*(D_{\infty})$. This self-similarity of $C^*(D_{\infty})$ is manifested by some dynamical properties of the joint spectrum.