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Chirally improving Wilson fermions II. Four-quark operators
High Energy Physics - Lattice · Submitted 2 Jul 2004
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim In this paper we discuss how the peculiar properties of twisted lattice QCD at maximal twist can be employed to set up a consistent computational scheme in which, despite the explicit breaking of chiral symmetry induced by the presence of the Wilson and mass terms in the action, it is possible to completely bypass the problem of wrong chirality and parity mixings in the computation of the CP-conserving matrix elements of the $\Delta S=1,2$ effective weak Hamiltonian and at the same time have a positive determinant for non-degenerate quarks as well as full O($a$) improvement in on-shell quantities with no need of improving the lattice action and the operators.
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In this paper we discuss how the peculiar properties of twisted lattice QCD at maximal twist can be employed to set up a consistent computational scheme in which, despite the explicit breaking of chiral symmetry induced by the presence of the Wilson and mass terms in the action, it is possible to completely bypass the problem of wrong chirality and parity mixings in the computation of the CP-conserving matrix elements of the $\Delta S=1,2$ effective weak Hamiltonian and at the same time have a positive determinant for non-degenerate quarks as well as full O($a$) improvement in on-shell quantities with no need of improving the lattice action and the operators.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | In this paper we discuss how the peculiar properties of twisted lattice QCD at maximal twist can be employed to set up a consistent computational scheme in which, despite the explicit breaking of chiral symmetry induced by the presence of the Wilson and mass terms in the action, it is possible to completely bypass the problem of wrong chirality and parity mixings in the computation of the CP-conserving matrix elements of the $\Delta S=1,2$ effective weak Hamiltonian and at the same time have a positive determinant for non-degenerate quarks as well as full O($a$) improvement in on-shell quantities with no need of improving the lattice action and the operators. | contribution 0.95 | 0.64 | 0.89 | asserted 0.69 |
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Original abstract
In this paper we discuss how the peculiar properties of twisted lattice QCD at maximal twist can be employed to set up a consistent computational scheme in which, despite the explicit breaking of chiral symmetry induced by the presence of the Wilson and mass terms in the action, it is possible to completely bypass the problem of wrong chirality and parity mixings in the computation of the CP-conserving matrix elements of the $\Delta S=1,2$ effective weak Hamiltonian and at the same time have a positive determinant for non-degenerate quarks as well as full O($a$) improvement in on-shell quantities with no need of improving the lattice action and the operators.
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References
How the literature uses it
82 arXiv papers cite this in 143 sentences
Papers whose main result relates to this one's
States the same result 1 paper
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We discuss how the peculiar properties of maximally twisted Wilson fermions can be exploited to set up a consistent LQCD computational scheme in which the CP-conserving matrix elements of the $\Delta S =1,2$ effective weak Hamiltonian can be evaluated without mixing with wrong-chirality and/or -parity operators.
Four quark operators in maximally twisted Wilson LQCD · 0.99
Papers citing it · 72 sentences without a confident label
Builds on it 1 paper
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We relied on the same mixed-action setup described in Refs. [ref] and evaluated, for each of the ensembles in TABLE [ref], the current-current correlator in Eq. ([ref]), extending to the $u̅s$ flavour channel the calculation performed in Ref. [ref] in the $u̅d$ sector (to which we refer for further technical details).
Inclusive hadronic decay rate of the $\tau$ lepton from lattice QCD: the $\bar u s$ flavour channel and the Cabibbo angle · Methods and Materials · 0.85
Uses its method or tool 56 papers
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In the valence sector we employ the Osterwalder-Seiler (OS) action [ref] .
Investigating a mixed action approach for {\eta} and {\eta}' mesons in Nf=2+1+1 lattice QCD · Lattice actions · 0.99
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For this reason we use a mixed action approach with the OS action [ref] in the valence sector and choose $D_ℓ^+$ in Eq. [ref] for both up and down quarks, so that the isospin symmetry is guaranteed in the valence sector.
Isospin-0 $\pi\pi$ s-wave scattering length from twisted mass lattice QCD · Finite volume spectrum · 0.92
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The valence quarks are twisted mass (TM) fermions [ref] , automatically $𝒪(a)$-improved by tuning the hopping parameter $κ$ to its critical value, such that the PCAC quark mass vanishes [ref] .
Step scaling in coordinate space: running of the quark mass · Introduction · 0.97
Cites it as support 2 papers
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We remark that the nonconserved local currents do not spoil the automatic $𝒪(a)$ improvement [ref] and the four-point function in Eq. ([ref]) is therefore $𝒪(a)$ improved.
Hadronic light-by-light contribution to the muon $g-2$ using twisted-mass fermions · Introduction · 0.97
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It has been shown in Ref. [ref] that this kind of mixed action preserves the automatic O$(a)$-improvement of physical observables, i.e. lattice artifacts, including those violating unitarity, scale as O$(a^2)$ implying that unitarity is safely recovered in the continuum limit.
$K$- and $D_{(s)}$-meson leptonic decay constants with physical light, strange and charm quarks by ETMC · Lattice action and simulations · 0.99
Cites it as background 2 papers
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The twisted mass formulation of Lattice QCD [ref] has been studied extensively with $N_f=2$ dynamical flavours by the European Twisted Mass (ETM) collaboration.
Light hadrons from Nf=2+1+1 dynamical twisted mass fermions · Introduction · 0.94
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The twisted mass formulation of Lattice QCD [ref] is being studied extensively with $N_f=2$ dynamical flavours by the European Twisted Mass (ETM) collaboration [ref] .
First results of ETMC simulations with Nf=2+1+1 maximally twisted mass fermions · Introduction · 0.97
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