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Twisted-mass lattice QCD with mass non-degenerate quarks
High Energy Physics - Lattice · Submitted 7 Nov 2003
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We show that in the case of maximal twist all these nice results can be extended to the more interesting case of a mass non-degenerate quark pair.
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The abstract, sentence by sentence
The maximally twisted lattice QCD action of an $SU_f(2)$ doublet of mass degenerate Wilson quarks gives rise to a real positive fermion determinant and it is invariant under the product of standard parity times the change of sign of the coefficient of the Wilson term. The existence of this spurionic symmetry implies that O($a$) improvement is either automatic or achieved through simple linear combinations of quantities taken with opposite external three-momenta. We show that in the case of maximal twist all these nice results can be extended to the more interesting case of a mass non-degenerate quark pair.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The maximally twisted lattice QCD action of an $SU_f(2)$ doublet of mass degenerate Wilson quarks gives rise to a real positive fermion determinant and it is invariant under the product of standard parity times the change of sign of the coefficient of the Wilson term. | background 0.99 | 0.14 | 0.06 | asserted 1.00 |
| s1 | The existence of this spurionic symmetry implies that O($a$) improvement is either automatic or achieved through simple linear combinations of quantities taken with opposite external three-momenta. | interpretation 0.61 | 0.14 | 0.08 | asserted 0.67 |
| s2 | We show that in the case of maximal twist all these nice results can be extended to the more interesting case of a mass non-degenerate quark pair. | contribution 0.61 | 0.92 | 0.88 | asserted 1.00 |
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The paper
Original abstract
The maximally twisted lattice QCD action of an $SU_f(2)$ doublet of mass degenerate Wilson quarks gives rise to a real positive fermion determinant and it is invariant under the product of standard parity times the change of sign of the coefficient of the Wilson term. The existence of this spurionic symmetry implies that O($a$) improvement is either automatic or achieved through simple linear combinations of quantities taken with opposite external three-momenta. We show that in the case of maximal twist all these nice results can be extended to the more interesting case of a mass non-degenerate quark pair.
Human review
References
How the literature uses it
55 arXiv papers cite this in 81 sentences
Papers citing it · 47 sentences without a confident label
Uses its method or tool 29 papers
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The latter are related to $μ_σ$ and $μ_δ$ via [ref] : [equation] where the $-$ sign corresponds to the strange and the $+$ sign to the charm.
Status of ETMC simulations with Nf=2+1+1 twisted mass fermions · Lattice action and simulation algorithm · 0.87
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for the light degenerate up/down doublet [ref] and the heavy non-degenerate strange/charm doublet [ref] respectively, where $D_W$ denotes the standard Wilson Dirac operator. $κ= 1 / (2 m_0 + 8)$ is tuned to maximal twist by requiring $m_χ^(l)^PCAC = 0$, which guarantees automatic $𝒪(a)$ improvement for physical quantities, e.g. the here considered kaon and $D$ meson masses.
Kaon and D meson masses with N_f = 2+1+1 twisted mass lattice QCD · Simulation setup · 0.86
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while for the $(c,s)$ doublet the twisted mass formulation for non-degenerate quarks of [ref] has been used:
Computing K and D meson masses with N_f = 2+1+1 twisted mass lattice QCD · $N_f = 2+1+1$ twisted mass lattice QCD · 0.97
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 1 paper
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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
Cites it as background 1 paper
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The generalisation to mass-non-degenerate flavour doublets exists [ref] , but lies beyond the scope of this paper.
Logarithmic corrections to O($a$) and O($a^2$) effects in lattice QCD with Wilson or Ginsparg-Wilson quarks · Wilson quarks with a chiral twist · 0.84
Discussion
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