2016
DOI: 10.1103/physrevd.94.054504
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Renormalization of domain-wall bilinear operators with short-distance current correlators

Abstract: We determine the renormalization constants for flavor non-singlet fermion bilinear operators of Möbius domain-wall fermions. The renormalization condition is imposed on the correlation functions in the coordinate space, such that the non-perturbative lattice calculation reproduces the perturbatively calculated counterpart at short distances. The perturbative expansion is precise as the coefficients are available up to O(α 4 s ). We employ 2 + 1-flavor lattice ensembles at three lattice spacings in the range 0.… Show more

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Cited by 31 publications
(49 citation statements)
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“…We remark that unlike in determinations of the renormalization constants [29][30][31], as long as 2 is within the above window, no knowledge on the functional form of ( ) is required to extract and˜. Moreover, short-distance lattice artefacts are much reduced within the above ratio.…”
Section: B Description Of the Methodsmentioning
confidence: 99%
“…We remark that unlike in determinations of the renormalization constants [29][30][31], as long as 2 is within the above window, no knowledge on the functional form of ( ) is required to extract and˜. Moreover, short-distance lattice artefacts are much reduced within the above ratio.…”
Section: B Description Of the Methodsmentioning
confidence: 99%
“…The spectral density observed on the lattice are multiplied by the renormalization factor Z S (2 GeV) to convert the results to those definition in the MS scheme. The renormalization factors are independently calculated in [8].…”
Section: Lattice Results and Chiral Fitsmentioning
confidence: 99%
“…Details of the lattice parameters are in [5], where a full description of this work is available. The same set of lattice ensembles is also used for calculations of other physical quantities such as the η meson mass [6], charm quark mass [7], short-distance current correlator [8,9], as well as heavy-light meson decay constants [10] and semileptonic decay form factors [11].…”
Section: Introductionmentioning
confidence: 99%
“…In principle, it is the same as that for the light-to-light renormalisation factor Z ll previously determined in [14]. In order to eliminate possible discretisation effects for large m h a, however, we adopt an improved estimate Z bl = √ Z bb Z ll determined nonperturbatively by demanding the matrix element B|V|B = 1.…”
Section: Correlator Fitsmentioning
confidence: 99%