David Preti
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View article: Non-perturbative renormalisation and improvement of non-singlet tensor currents in Nf = 3 QCD
Non-perturbative renormalisation and improvement of non-singlet tensor currents in Nf = 3 QCD Open
View article: Hadronic physics from a Wilson fermion mixed-action approach: charm quark mass and $$D_{(s)}$$ meson decay constants
Hadronic physics from a Wilson fermion mixed-action approach: charm quark mass and $$D_{(s)}$$ meson decay constants Open
View article: Hadronic physics from a Wilson fermion mixed-action approach: charm quark mass and $D_{(s)}$ meson decay constants
Hadronic physics from a Wilson fermion mixed-action approach: charm quark mass and $D_{(s)}$ meson decay constants Open
We present our first set of results for charm physics, using the mixed-action setup introduced in a companion paper [1]. Maximally twisted Wilson valence fermions are used on a sea of non-perturbatively O(a)-improved Wilson fermions, made …
View article: Non-perturbative renormalisation and improvement of non-singlet tensor currents in $N_\mathrm{f}=3$ QCD
Non-perturbative renormalisation and improvement of non-singlet tensor currents in $N_\mathrm{f}=3$ QCD Open
Hadronic matrix elements involving tensor currents play an important rôle 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 (anom…
View article: Light meson physics and scale setting from a mixed action with Wilson twisted mass valence quarks
Light meson physics and scale setting from a mixed action with Wilson twisted mass valence quarks Open
We consider a mixed action approach where valence Wilson twisted mass (Wtm) fermions at maximal twist are combined with CLS ensembles consisting of $N_f$=2+1 flavours of O($a$)-improved Wilson sea quarks. We present an update of the result…
View article: Charm physics with a tmQCD mixed action
Charm physics with a tmQCD mixed action Open
We report on our ongoing determination of the charm quark mass and the masses and decay constants of various charmed mesons, obtained within a mixed-action setup. We employ $N_f=2+1$ CLS ensembles combined with a Wilson twisted mass valenc…
View article: Calculation of the running coupling in non-Abelian gauge theories from Jarzynski's equality
Calculation of the running coupling in non-Abelian gauge theories from Jarzynski's equality Open
We discuss the theoretical foundations of non-equilibrium Monte Carlo simulations based on Jarzynski's equality and present, as an example of application, the determination of the running coupling in the Schrödinger-functional scheme.
View article: Calculation of the running coupling in non-Abelian gauge theories from Jarzynski's equality
Calculation of the running coupling in non-Abelian gauge theories from Jarzynski's equality Open
We discuss the theoretical foundations of non-equilibrium Monte Carlo simulations based on Jarzynski's equality and present, as an example of application, the determination of the running coupling in the Schrödinger-functional scheme.
View article: Non-perturbative renormalization of O($a$) improved tensor currents
Non-perturbative renormalization of O($a$) improved tensor currents Open
We present our progress in the non-perturbative O(a) improvement and renormalization of tensor currents in three-flavor lattice QCD with Wilson-clover fermions and tree-level Symanzik improved gauge action. The mass-independent O(a) improv…
View article: Non-perturbative renormalization of $O(a)$ improved tensor currents
Non-perturbative renormalization of $O(a)$ improved tensor currents Open
We present our progress in the non-perturbative $O(a)$ improvement and renormalization of tensor currents in three-flavor lattice QCD with Wilson-clover fermions and tree-level Symanzik improved gauge action. The mass-independent $O(a)$ im…
View article: Strong dynamics with matter in multiple representations: $$\mathrm {SU}(4)$$ gauge theory with fundamental and sextet fermions
Strong dynamics with matter in multiple representations: $$\mathrm {SU}(4)$$ gauge theory with fundamental and sextet fermions Open
View article: Light and strange quark masses for $N_f = 2 + 1$ simulations with Wilson fermions
Light and strange quark masses for $N_f = 2 + 1$ simulations with Wilson fermions Open
We present a preliminary analysis of the $u/d$ and $s$ quark masses, extracted using the PCAC quark masses reported in PRD 95 (2017) 074504. The data is based on the CLS $N_f = 2 + 1$ simulations with Wilson/Clover quarks and Lüscher-Weisz…
View article: Heavy-quark physics with a tmQCD valence action
Heavy-quark physics with a tmQCD valence action Open
We introduce a mixed-action approach based on CLS ensembles, where a valence $N_f$=2+1+1 Twisted Mass QCD action is combined with the $N_f$=2+1 non-perturbatively O$(a)$-improved Wilson sea sector. We show that for maximally twisted valenc…
View article: Matching of $N_f=2+1$ CLS ensembles to a tmQCD valence sector
Matching of $N_f=2+1$ CLS ensembles to a tmQCD valence sector Open
A mixed action composed of valence quark flavours regularized with a fully-twisted tmQCD action and of $N_f=2+1$ flavours of non-perturbatively ${\rm O}(a)$-improved Wilson sea quarks is described. Two procedures for the matching of sea an…
View article: First results for charm physics with a tmQCD valence action
First results for charm physics with a tmQCD valence action Open
We present preliminary results in the charm sector from a mixed-action setup, in which CLS $N_f=2+1$ ensembles are combined with a Wilson twisted mass valence action. We study the continuum and chiral limits of charm quark observables such…
View article: Light and strange quark masses from $N_f=2+1$ simulations with Wilson fermions
Light and strange quark masses from $N_f=2+1$ simulations with Wilson fermions Open
We present a nearly final analysis of the $u/d$ and $s$ quark masses, extracted using the PCAC quark masses reported in [PRD 95 (2017) 074504]. The data is based on the CLS $N_f = 2 + 1$ simulations with Wilson/Clover quarks and Lüscher-We…
View article: Matching of $N_f=2+1$ CLS ensembles to a tmQCD valence sector
Matching of $N_f=2+1$ CLS ensembles to a tmQCD valence sector Open
A mixed action composed of valence quark flavours regularized with a fully-twisted tmQCD action and of $N_f=2+1$ flavours of non-perturbatively ${\rm O}(a)$-improved Wilson sea quarks is described. Two procedures for the matching of sea an…
View article: First results for charm physics with a tmQCD valence action
First results for charm physics with a tmQCD valence action Open
We present preliminary results in the charm sector from a mixed-action setup, in which CLS $N_f=2+1$ ensembles are combined with a Wilson twisted mass valence action. We study the continuum and chiral limits of charm quark observables such…
View article: Erratum to: On the perturbative renormalization of four-quark operators for new physics
Erratum to: On the perturbative renormalization of four-quark operators for new physics Open
\n This erratum concerns the correction of some typographic errors appearing in the second and third sections of the article. The errors do not affect any of the results presented.\n
View article: On the perturbative renormalization of four-quark operators for new physics
On the perturbative renormalization of four-quark operators for new physics Open
View article: Controlling quark mass determinations non-perturbatively in three-flavour QCD
Controlling quark mass determinations non-perturbatively in three-flavour QCD Open
\nThe determination of quark masses from lattice QCD simulations requires a non-perturbative renormalization procedure and subsequent scale evolution to high energies, where a conversion to the commonly used $\\overline {{\\rm{MS}}} $ sche…
View article: Non-perturbative running of quark masses in three-flavour QCD
Non-perturbative running of quark masses in three-flavour QCD Open
We present our preliminary results for the computation of the non-perturbative running of renormalized quark masses in $N_f = 3$ QCD, between the electroweak and hadronic scales, using standard finite-size scaling techniques. The computati…
View article: On the perturbative renormalisation of four-quark operators for new physics
On the perturbative renormalisation of four-quark operators for new physics Open
We discuss the renormalisation properties of the full set of $ΔF=2$ operators involved in BSM processes, including the definition of RGI versions of operators that exhibit mixing under RG transformations. As a first step for a fully non-pe…
View article: On the perturbative renormalisation of four-quark operators for new\n physics
On the perturbative renormalisation of four-quark operators for new\n physics Open
We discuss the renormalisation properties of the full set of $\\Delta F=2$\noperators involved in BSM processes, including the definition of RGI versions\nof operators that exhibit mixing under RG transformations. As a first step for\na fu…
View article: Non-perturbative running of quark masses in three-flavour QCD
Non-perturbative running of quark masses in three-flavour QCD Open
We present our preliminary results for the computation of the non-perturbative running of renormalized quark masses in $N_f = 3$ QCD, between the electroweak and hadronic scales, using standard finite-size scaling techniques. The computati…
View article: Prospects and status of quark mass renormalization in three-flavour QCD
Prospects and status of quark mass renormalization in three-flavour QCD Open
We present the current status of a revised strategy to compute the running of renormalized quark masses in QCD with three flavours of massless O(a) improved Wilson quarks. The strategy employed uses the standard finite-size scaling method …
View article: Non-perturbative renormalization of tensor bilinears in Schrodinger Functional schemes
Non-perturbative renormalization of tensor bilinears in Schrodinger Functional schemes Open
We present preliminary result for the study of the renormalization group evolution of tensor bilinears in Schrödinger Functional (SF) schemes for N f = 0 and N f = 2 QCD with non-perturbatively O(a)-improved Wilson fermions.First N f = 2 +…
View article: Non-perturbative renormalization of tensor bilinears in Schrödinger Functional schemes
Non-perturbative renormalization of tensor bilinears in Schrödinger Functional schemes Open
We present preliminary result for the study of the renormalization group evolution of tensor bilinears in Schrödinger Functional (SF) schemes for $N_f=0$ and $N_f=2$ QCD with non-perturbatively $\mathcal{O}(a)$-improved Wilson fermions. Fi…
View article: Non-perturbative renormalization of tensor bilinears in Schr\\"odinger\n Functional schemes
Non-perturbative renormalization of tensor bilinears in Schr\\"odinger\n Functional schemes Open
We present preliminary result for the study of the renormalization group\nevolution of tensor bilinears in Schr\\"odinger Functional (SF) schemes for\n$N_f=0$ and $N_f=2$ QCD with non-perturbatively $\\mathcal{O}(a)$-improved\nWilson fermi…
View article: Prospects and status of quark mass renormalization in three-flavour QCD
Prospects and status of quark mass renormalization in three-flavour QCD Open
We present the current status of a revised strategy to compute the running of renormalized quark masses in QCD with three flavours of massless O(a) improved Wilson quarks. The strategy employed uses the standard finite-size scaling method …