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Functional Equations and Pole Structure of the Bartholdi Zeta Function (2408.04952v1)

Published 9 Aug 2024 in math.CO, hep-lat, hep-th, math-ph, and math.MP

Abstract: In this paper, we investigate the Bartholdi zeta function on a connected simple digraph with $n_V$ vertices and $n_E$ edges. We derive a functional equation for the Bartholdi zeta function $\zeta_G(q,u)$ on a regular graph $G$ with respect to the bump parameter $u$. We also find an equivalence between the Bartholdi zeta function with a specific value of $u$ and the Ihara zeta function at $u=0$. We determine bounds of the critical strip of $\zeta_G(q,u)$ for a general graph. If $G$ is a $(t+1)$-regular graph, the bounds are saturated and $q=(1-u){-1}$ and $q=(t+u){-1}$ are the poles at the boundaries of the critical strip for $u\ne 1, -t$. When $G$ is the regular graph and the spectrum of the adjacency matrix satisfies a certain condition, $\zeta_G(q,u)$ satisfies the so-called Riemann hypothesis. For $u \ne 1$, $q=\pm(1-u){-1}$ are poles of $\zeta_G(q,u)$ unless $G$ is tree. Although the order of the pole at $q=(1-u){-1}$ is $n_E-n_V+1$ if $u\ne u_* \equiv 1-\frac{n_E}{n_V}$, it is enhanced at $u=u_$. In particular, if the Moore-Penrose inverse of the incidence matrix $L+$ and the degree vector $\vec{d}$ satisfy the condition $|L+ \vec{d}|2\ne n_E$, the order of the pole at $q=(1-u){-1}$ increases only by one at $u=u_$. The order of the pole at $q=-(1-u){-1}$ coincides with that at $q=(1-u){-1}$ if $G$ is bipartite and is $n_E-n_V$ otherwise.

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