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Gauge invariant non-perturbative Wilson action in quantum electrodynamics

Sorato Nagao, Hiroshi Suzuki

Abstract

By employing the gradient flow exact renormalization group (GFERG), we study the renormalization group (RG) flow of a manifestly gauge or BRST invariant non-perturbative ansatz of the 1PI Wilson action in quantum electrodynamics. The gauge invariance of the Wilson action is \emph{exactly\/} preserved under the RG flow. We explicitly solve the GFERG equation in the leading and partially the next to leading orders of the large $N_f$ approximation, where $N_f$ is the number of flavors. We obtain gauge invariant critical exponents and the gauge invariant 1PI Wilson action at an infrared (IR) fixed point for~$D<4$, where $D$ is the spacetime dimension.

Gauge invariant non-perturbative Wilson action in quantum electrodynamics

Abstract

By employing the gradient flow exact renormalization group (GFERG), we study the renormalization group (RG) flow of a manifestly gauge or BRST invariant non-perturbative ansatz of the 1PI Wilson action in quantum electrodynamics. The gauge invariance of the Wilson action is \emph{exactly\/} preserved under the RG flow. We explicitly solve the GFERG equation in the leading and partially the next to leading orders of the large approximation, where is the number of flavors. We obtain gauge invariant critical exponents and the gauge invariant 1PI Wilson action at an infrared (IR) fixed point for~, where is the spacetime dimension.
Paper Structure (17 sections, 129 equations, 2 figures)

This paper contains 17 sections, 129 equations, 2 figures.

Figures (2)

  • Figure 1: The function $\mathcal{C}(k^2)$\ref{['eq:(4.17)']} as the function of $k^2$.
  • Figure 2: The function $\mathcal{K}_\tau(k^2)$ in the 1PI Wilson action \ref{['eq:(3.5)']} at the IR fixed point in the leading large $N_f$ approximation; the horizontal axis is $k^2$.