Hadronic physics from a Wilson fermion mixed-action approach: Setup and scale setting

TL;DR

This paper introduces a mixed-action lattice QCD approach combining Wilson-type quarks in sea and valence sectors, and demonstrates its effectiveness through scale setting and universality tests across multiple lattice parameters.

Contribution

The study develops a mixed-action setup with Wilson fermions, details the matching strategy for sea and valence quarks, and performs a precise scale setting using multiple methods, enhancing control over systematic uncertainties.

Findings

Successful universality test between mixed-action and unitary setups.

Precise determination of the gradient flow scale $t_0$.

Enhanced systematic control by combining different scale setting methods.

Abstract

We introduce a lattice QCD mixed action approach that employs Wilson-type quarks in the sea and valence sectors. The sea sector is based on gauge ensembles with $N_{\rm f}=2+1$ flavours of non-perturbatively O($a$)-improved Wilson fermions generated by the Coordinated Lattice Simulations (CLS) initiative. The parameter space of the considered ensembles encompasses five values of the lattice spacing, a range of pion masses extending down to the physical point, and large physical volumes. In the valence sector, we employ Wilson twisted-mass fermions at maximal twist, using the same massless Wilson-Dirac operator in both the sea and valence sectors. We describe the strategy applied for the required matching of the sea and valence quark masses along the target renormalised chiral trajectory. A precise universality test is then conducted by comparing the continuum-limit results of the mixed-action approach and of the unitary setup, in which the same Wilson fermion regularisation is employed in the sea and in the valence. As a key application, we conduct a scale setting procedure based on lattice determinations of the masses and decay constants of the pion and kaon, as well as the gradient flow scale $t_0$. The scale setting can consequently be performed in three distinct ways, utilising the unitary setup, the mixed action approach, and their combination. We observe that the latter combination results in enhanced control of the systematic uncertainties, thereby yielding a precise determination of the physical value of $t_0$.