Renormalization of local quark-bilinear operators for Nf=3 flavors of SLiNC fermions

TL;DR

This paper non-perturbatively computes renormalization factors for local quark-bilinear operators in Nf=3 SLiNC fermions, addressing chiral and continuum extrapolations, lattice artifacts, and scheme conversions to ensure precise results.

Contribution

It introduces a comprehensive non-perturbative renormalization procedure for Nf=3 SLiNC fermions, including systematic artifact subtraction and scheme translation.

Findings

Renormalization factors are computed at multiple scales and schemes.

Lattice artifacts are effectively reduced using perturbative subtraction methods.

Systematic errors are thoroughly analyzed and minimized.

Abstract

The renormalization factors of local quark-bilinear operators are computed non-perturbatively for $N_f=3$ flavors of SLiNC fermions, with emphasis on the various procedures for the chiral and continuum extrapolations. The simulations are performed at a lattice spacing $a=0.074$ fm, and for five values of the pion mass in the range of 290-465 MeV, allowing a safe and stable chiral extrapolation. Emphasis is given in the subtraction of the well-known pion pole which affects the renormalization factor of the pseudoscalar current. We also compute the inverse propagator and the Green's functions of the local bilinears to one loop in perturbation theory. We investigate lattice artifacts by computing them perturbatively to second order as well as to all orders in the lattice spacing. The renormalization conditions are defined in the RI$'$-MOM scheme, for both the perturbative and non-perturbative results. The renormalization factors, obtained at different values of the renormalization scale, are translated to the ${\bar{\rm MS}}$ scheme and are evolved perturbatively to 2 GeV. Any residual dependence on the initial renormalization scale is eliminated by an extrapolation to the continuum limit. We also study the various sources of systematic errors. Particular care is taken in correcting the non-perturbative estimates by subtracting lattice artifacts computed to one loop perturbation theory using the same action. We test two different methods, by subtracting either the ${\cal O}(g^2\,a^2)$ contributions, or the complete (all orders in $a$) one-loop lattice artifacts.