Hadronic matrix elements involving tensor currents play an important role in decays that allow to probe the consistency of the Standard Model via precision lattice QCD calculations. The non-singlet tensor current is a scale-dependent (anomalous) quantity. We fully resolve its renormalisation group (RG) running in the continuum by carrying out a recursive finite-size scaling technique. In this way ambiguities due to a perturbative RG running and matching to lattice data at low energies are eliminated. We provide the total renormalisation factor at a hadronic scale of 233 MeV, which converts the bare current into its RG-invariant form. Our calculation features three flavours of O(a) improved Wilson fermions and tree-level Symanzik-improved gauge action. We employ the (massless) Schr & ouml;dinger functional renormalisation scheme throughout and present the first non-perturbative determination of the Symanzik counterterm c(T) derived from an axial Ward identity. We elaborate on various details of our calculations, including two different renormalisation conditions.
Non-perturbative renormalisation and improvement of non-singlet tensor currents in Nf = 3 QCD
Panero, Marco;Preti, David
2024-01-01
Abstract
Hadronic matrix elements involving tensor currents play an important role in decays that allow to probe the consistency of the Standard Model via precision lattice QCD calculations. The non-singlet tensor current is a scale-dependent (anomalous) quantity. We fully resolve its renormalisation group (RG) running in the continuum by carrying out a recursive finite-size scaling technique. In this way ambiguities due to a perturbative RG running and matching to lattice data at low energies are eliminated. We provide the total renormalisation factor at a hadronic scale of 233 MeV, which converts the bare current into its RG-invariant form. Our calculation features three flavours of O(a) improved Wilson fermions and tree-level Symanzik-improved gauge action. We employ the (massless) Schr & ouml;dinger functional renormalisation scheme throughout and present the first non-perturbative determination of the Symanzik counterterm c(T) derived from an axial Ward identity. We elaborate on various details of our calculations, including two different renormalisation conditions.File | Dimensione | Formato | |
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