English

Functional Equations and Pole Structure of the Bartholdi Zeta Function

Combinatorics 2024-08-12 v1 High Energy Physics - Lattice High Energy Physics - Theory Mathematical Physics math.MP

Abstract

In this paper, we investigate the Bartholdi zeta function on a connected simple digraph with nVn_V vertices and nEn_E edges. We derive a functional equation for the Bartholdi zeta function ζG(q,u)\zeta_G(q,u) on a regular graph GG with respect to the bump parameter uu. We also find an equivalence between the Bartholdi zeta function with a specific value of uu and the Ihara zeta function at u=0u=0. We determine bounds of the critical strip of ζG(q,u)\zeta_G(q,u) for a general graph. If GG is a (t+1)(t+1)-regular graph, the bounds are saturated and q=(1u)1q=(1-u)^{-1} and q=(t+u)1q=(t+u)^{-1} are the poles at the boundaries of the critical strip for u1,tu\ne 1, -t. When GG is the regular graph and the spectrum of the adjacency matrix satisfies a certain condition, ζG(q,u)\zeta_G(q,u) satisfies the so-called Riemann hypothesis. For u1u \ne 1, q=±(1u)1q=\pm(1-u)^{-1} are poles of ζG(q,u)\zeta_G(q,u) unless GG is tree. Although the order of the pole at q=(1u)1q=(1-u)^{-1} is nEnV+1n_E-n_V+1 if uu1nEnVu\ne u_* \equiv 1-\frac{n_E}{n_V}, it is enhanced at u=uu=u_*. In particular, if the Moore-Penrose inverse of the incidence matrix L+L^+ and the degree vector d\vec{d} satisfy the condition L+d2nE|L^+ \vec{d}|^2\ne n_E, the order of the pole at q=(1u)1q=(1-u)^{-1} increases only by one at u=uu=u_*. The order of the pole at q=(1u)1q=-(1-u)^{-1} coincides with that at q=(1u)1q=(1-u)^{-1} if GG is bipartite and is nEnVn_E-n_V otherwise.

Keywords

Cite

@article{arxiv.2408.04952,
  title  = {Functional Equations and Pole Structure of the Bartholdi Zeta Function},
  author = {So Matsuura and Kazutoshi Ohta},
  journal= {arXiv preprint arXiv:2408.04952},
  year   = {2024}
}

Comments

30 pages

R2 v1 2026-06-28T18:08:28.274Z