Functional Equations and Pole Structure of the Bartholdi Zeta Function
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 betwe...
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creator | Matsuura, So Ohta, Kazutoshi |
description | 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. |
doi_str_mv | 10.48550/arxiv.2408.04952 |
format | Article |
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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.</description><identifier>DOI: 10.48550/arxiv.2408.04952</identifier><language>eng</language><subject>Mathematics - Combinatorics ; Mathematics - Mathematical Physics ; Physics - High Energy Physics - Lattice ; Physics - High Energy Physics - Theory ; Physics - Mathematical Physics</subject><creationdate>2024-08</creationdate><rights>http://arxiv.org/licenses/nonexclusive-distrib/1.0</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,780,885</link.rule.ids><linktorsrc>$$Uhttps://arxiv.org/abs/2408.04952$$EView_record_in_Cornell_University$$FView_record_in_$$GCornell_University$$Hfree_for_read</linktorsrc><backlink>$$Uhttps://doi.org/10.48550/arXiv.2408.04952$$DView paper in arXiv$$Hfree_for_read</backlink></links><search><creatorcontrib>Matsuura, So</creatorcontrib><creatorcontrib>Ohta, Kazutoshi</creatorcontrib><title>Functional Equations and Pole Structure of the Bartholdi Zeta Function</title><description>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.</description><subject>Mathematics - Combinatorics</subject><subject>Mathematics - Mathematical Physics</subject><subject>Physics - High Energy Physics - Lattice</subject><subject>Physics - High Energy Physics - Theory</subject><subject>Physics - Mathematical Physics</subject><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><sourceid>GOX</sourceid><recordid>eNpjYJA0NNAzsTA1NdBPLKrILNMzMjGw0DMwsTQ14mRwcyvNSy7JzM9LzFFwLSxNBDGLFRLzUhQC8nNSFYJLikqTS0qLUhXy0xRKMlIVnBKLSjLyc1IyFaJSSxIVYLp5GFjTEnOKU3mhNDeDvJtriLOHLtjG-IKizNzEosp4kM3xYJuNCasAAG-mOOk</recordid><startdate>20240809</startdate><enddate>20240809</enddate><creator>Matsuura, So</creator><creator>Ohta, Kazutoshi</creator><scope>AKZ</scope><scope>GOX</scope></search><sort><creationdate>20240809</creationdate><title>Functional Equations and Pole Structure of the Bartholdi Zeta Function</title><author>Matsuura, So ; Ohta, Kazutoshi</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-arxiv_primary_2408_049523</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2024</creationdate><topic>Mathematics - Combinatorics</topic><topic>Mathematics - Mathematical Physics</topic><topic>Physics - High Energy Physics - Lattice</topic><topic>Physics - High Energy Physics - Theory</topic><topic>Physics - Mathematical Physics</topic><toplevel>online_resources</toplevel><creatorcontrib>Matsuura, So</creatorcontrib><creatorcontrib>Ohta, Kazutoshi</creatorcontrib><collection>arXiv Mathematics</collection><collection>arXiv.org</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Matsuura, So</au><au>Ohta, Kazutoshi</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Functional Equations and Pole Structure of the Bartholdi Zeta Function</atitle><date>2024-08-09</date><risdate>2024</risdate><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.</abstract><doi>10.48550/arxiv.2408.04952</doi><oa>free_for_read</oa></addata></record> |
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subjects | Mathematics - Combinatorics Mathematics - Mathematical Physics Physics - High Energy Physics - Lattice Physics - High Energy Physics - Theory Physics - Mathematical Physics |
title | Functional Equations and Pole Structure of the Bartholdi Zeta Function |
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