Fermions and Zeta Function on the Graph

TL;DR

This paper introduces a new fermionic model on graphs where the partition function relates to the inverse of the graph zeta function, revealing insights into fermionic cycles, gauge theories, and fermion doubling issues.

Contribution

It develops a novel fermionic model on graphs using deformed incidence matrices, connects it to the graph zeta function, and constructs gauge theories with fermions on general graphs.

Findings

Coefficients of the inverse zeta function count fermionic cycles.

Fermion doubling is absent, allowing overlap fermions on graphs.

The model links to statistical models via winding numbers and pole distributions.

Abstract

We propose a novel fermionic model on the graphs. The Dirac operator of the model consists of deformed incidence matrices on the graph and the partition function is given by the inverse of the graph zeta function. We find that the coefficients of the inverse of the graph zeta function, which is a polynomial of finite degree in the coupling constant, count the number of fermionic cycles on the graph. We also construct the model on grid graphs by using the concept of the covering graph and the Artin-Ihara $L$-function. In connection with this, we show that the fermion doubling is absent, and the overlap fermions can be constructed on a general graph. Furthermore, we relate our model to statistical models by introducing the winding number around cycles, where the distribution of the poles of the graph zeta function (the zeros of the partition function) plays a crucial role. Finally, we formulate gauge theory including fermions on the graph from the viewpoint of the covering graph derived from the gauge group in a unified way.