Two-loop mass anomalous dimension in reduced quantum electrodynamics and application to dynamical fermion mass generation

TL;DR

This paper calculates the two-loop mass anomalous dimension in reduced QED models and applies it to analyze dynamical fermion mass generation, providing gauge-invariant critical parameters and confirming results with existing numerical and analytical methods.

Contribution

It introduces a gauge-invariant gap equation using the two-loop anomalous dimension to study dynamical mass generation in reduced QED models, with analytical expressions for critical coupling and flavor number.

Findings

Analytical expression for the gauge-invariant critical coupling constant.

Agreement with previous truncated Schwinger-Dyson equation analyses.

Good quantitative match with numerical results for QED$_4$.

Abstract

We consider reduced quantum electrodynamics (RQED$_{d_\gamma,d_e}$) a model describing fermions in a $d_e$-dimensional space-time and interacting via the exchange of massless bosons in $d_\gamma$-dimensions ($d_e \leq d_\gamma$). We compute the two-loop mass anomalous dimension, $\gamma_m$, in general RQED$_{4,d_e}$ with applications to RQED$_{4,3}$ and QED$_4$. We then proceed on studying dynamical (parity-even) fermion mass generation in RQED$_{4,d_e}$ by constructing a fully gauge-invariant gap equation for RQED$_{4,d_e}$ with $\gamma_m$ as the only input. This equation allows for a straightforward analytic computation of the gauge-invariant critical coupling constant, $\alpha_c$, which is such that a dynamical mass is generated for $\alpha_r > \alpha_c$, where $\alpha_r$ is the renormalized coupling constant, as well as the gauge-invariant critical number of fermion flavours, $N_c$, which is such that $\alpha_c \rightarrow \infty$ and a dynamical mass is generated for $N < N_c$. For RQED$_{4,3}$, our results are in perfect agreement with the more elaborate analysis based on the resolution of truncated Schwinger-Dyson equations at two-loop order. In the case of QED$_4$, our analytical results (that use state of the art five-loop expression for $\gamma_m$) are in good quantitative agreement with those obtained from numerical approaches.