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Chirally improving Wilson fermions - I. O(a) improvement
High Energy Physics - Lattice · Submitted 12 Jun 2003
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We show that it is possible to improve the chiral behaviour and the approach to the continuum limit of correlation functions in lattice QCD with Wilson fermions by taking arithmetic averages of correlators computed in theories regularized with Wilson terms of opposite sign.
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We show that it is possible to improve the chiral behaviour and the approach to the continuum limit of correlation functions in lattice QCD with Wilson fermions by taking arithmetic averages of correlators computed in theories regularized with Wilson terms of opposite sign. Improved hadronic masses and matrix elements can be obtained by similarly averaging the corresponding physical quantities separately computed within the two regularizations. To deal with the problems related to the spectrum of the Wilson--Dirac operator, which are particularly worrisome when Wilson and mass terms are such as to give contributions of opposite sign to the real part of the eigenvalues, we propose to use twisted-mass lattice QCD for the actual computation of the quantities taking part to the averages. The choice $\pm \pi/2$ for the twisting angle is particularly interesting, as O($a$) improved estimates of physical quantities can be obtained even without averaging data from lattice formulations with opposite Wilson terms. In all cases little or no extra computing power is necessary, compared to simulations with standard Wilson fermions or twisted-mass lattice QCD.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We show that it is possible to improve the chiral behaviour and the approach to the continuum limit of correlation functions in lattice QCD with Wilson fermions by taking arithmetic averages of correlators computed in theories regularized with Wilson terms of opposite sign. | contribution 0.68 | 0.87 | 0.85 | asserted 0.67 |
| s1 | Improved hadronic masses and matrix elements can be obtained by similarly averaging the corresponding physical quantities separately computed within the two regularizations. | result 0.43 | 0.48 | 0.11 | hedged possibility 0.51 |
| s2 | To deal with the problems related to the spectrum of the Wilson--Dirac operator, which are particularly worrisome when Wilson and mass terms are such as to give contributions of opposite sign to the real part of the eigenvalues, we propose to use twisted-mass lattice QCD for the actual computation of the quantities taking part to the averages. | method 0.87 | 0.39 | 0.09 | hedged possibility 0.69 |
| s3 | The choice $\pm \pi/2$ for the twisting angle is particularly interesting, as O($a$) improved estimates of physical quantities can be obtained even without averaging data from lattice formulations with opposite Wilson terms. | result 0.62 | 0.65 | 0.21 | asserted 0.78 |
| s4 | In all cases little or no extra computing power is necessary, compared to simulations with standard Wilson fermions or twisted-mass lattice QCD. | interpretation 0.56 | 0.46 | 0.06 | asserted 0.95 |
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Original abstract
We show that it is possible to improve the chiral behaviour and the approach to the continuum limit of correlation functions in lattice QCD with Wilson fermions by taking arithmetic averages of correlators computed in theories regularized with Wilson terms of opposite sign. Improved hadronic masses and matrix elements can be obtained by similarly averaging the corresponding physical quantities separately computed within the two regularizations. To deal with the problems related to the spectrum of the Wilson--Dirac operator, which are particularly worrisome when Wilson and mass terms are such as to give contributions of opposite sign to the real part of the eigenvalues, we propose to use twisted-mass lattice QCD for the actual computation of the quantities taking part to the averages. The choice $\pm \pi/2$ for the twisting angle is particularly interesting, as O($a$) improved estimates of physical quantities can be obtained even without averaging data from lattice formulations with opposite Wilson terms. In all cases little or no extra computing power is necessary, compared to simulations with standard Wilson fermions or twisted-mass lattice QCD.
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References
How the literature uses it
161 arXiv papers cite this in 259 sentences
Papers whose main result relates to this one's
States the same result 1 paper
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It is possible to improve the chiral behaviour and the approach to the continuum limit of correlation functions in lattice QCD with standard and twisted Wilson fermions by taking arithmetic averages of correlators computed in theories regularized with Wilson terms of opposite sign.
Papers citing it · 159 sentences without a confident label
Uses its method or tool 76 papers
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Once the bare charm quark mass $μ_c$ is extracted, we renormalise it in the RI-MOM scheme: $m^RI-MOM_c = Z^RI-MOM_μμ_c$ where $Z^RI-MOM_μ=1/Z^RI-MOM_P$ in TmQCD [ref] .
Twisted mass QCD in the charm sector · Charm quark mass · 0.97
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We calculate for the first time the bare matrix elements of all the relevant 4-quark operators for one ensemble of $N_f=2+1+1$ twisted mass fermions [ref] at maximal twist [ref] at pion mass $M_π = 260$ MeV generated by the Extended Twisted Mass Collaboration (ETMC) [ref] .
Hadronic Parity Violation from Twisted Mass Lattice QCD · Introduction · 0.83
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According to Ref. [ref] , in order to guarantee the $O(a)$ improvement of the extracted matrix elements we consider the two kinematics with opposite spatial momenta of the parent and child mesons and perform the following average:
Tensor form factor of $D \to \pi(K) \ell \nu$ and $D \to \pi(K) \ell \ell$ decays with $N_f=2+1+1$ twisted-mass fermions · Lattice calculation of the tensor matrix elements · 0.99
Uses its data or values 1 paper
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In our work we used two gauge ensembles generated by the JLQCD collaboration [ref] and by the ETM collaboration [ref] , which use Domain Wall fermions and Twisted-Mass Wilson fermions respectively.
Inclusive semileptonic $B$-decays from lattice QCD · Lattice computation · 0.96
Cites it as support 2 papers
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It depends on [equation] The expression for $M_π^2$ explicitly verifies that $O(a)$-improvement of the pion mass requires both twist angles to be at maximal twist [ref] .
Twisted mass chiral perturbation theory for 2+1+1 quark flavours · Pion masses · 0.98
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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
Cites it as background 11 papers
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The presence of lattice artifacts brings in new types of mass terms, one of which is often referred to as a “twisted” mass [ref] .
Effective potentials, thermodynamics, and twisted mass quarks · Introduction · 0.95
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Moreover, another class of mixed actions involves using variants of the sea action in the valence sector, such as Osterwalder-Seiler quarks on a twisted mass sea [ref] .], namely using maximally twisted mass fermions [ref] in the sea sector and overlap fermions in the valence sector.
Overlap valence quarks on a twisted mass sea: a case study for mixed action Lattice QCD · Introduction · 0.92
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In Sec. [ref] we move onto twisted-mass fermions, focusing first on the phase diagram and pion masses in the case of maximal twist, where most simulations have been done because of the property of automatic $𝒪(a)$ improvement [ref] .
Phase diagram of non-degenerate twisted mass fermions · Introduction · 0.84
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