2016
DOI: 10.1007/jhep01(2016)093
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Non-perturbative tests of continuum HQET through small-volume two-flavour QCD

Abstract: Abstract:We study the heavy quark mass dependence of selected observables constructed from heavy-light meson correlation functions in small-volume two-flavour lattice QCD after taking the continuum limit. The light quark mass is tuned to zero, whereas the range of available heavy quark masses m h covers a region extending from around the charm to beyond the bottom quark mass scale. This allows entering the asymptotic mass-scaling regime as 1/m h → 0 and performing well-controlled extrapolations to the infinite… Show more

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Cited by 6 publications
(7 citation statements)
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“…Although not necessary for O(a) improvement of physical quantities [23] (at maximal twist), it has been shown to reduce O(a 2 ) artifacts in some cases [25], and more importantly gives us access to the wide range of renormalization factors that have been determined non-perturbatively in the past. In particular we benefit from the knowledge of the critical mass m cr [26,27] and the axial current and pseudoscalar density renormalization factors Z A [28][29][30] and Z P [26,31]. Since one of our goals is a detailed understanding of charm related lattice artifacts, we simulate also at very fine lattice spacings, much finer than what is currently feasible in simulations that include light quarks.…”
Section: Actions and Algorithmsmentioning
confidence: 99%
See 1 more Smart Citation
“…Although not necessary for O(a) improvement of physical quantities [23] (at maximal twist), it has been shown to reduce O(a 2 ) artifacts in some cases [25], and more importantly gives us access to the wide range of renormalization factors that have been determined non-perturbatively in the past. In particular we benefit from the knowledge of the critical mass m cr [26,27] and the axial current and pseudoscalar density renormalization factors Z A [28][29][30] and Z P [26,31]. Since one of our goals is a detailed understanding of charm related lattice artifacts, we simulate also at very fine lattice spacings, much finer than what is currently feasible in simulations that include light quarks.…”
Section: Actions and Algorithmsmentioning
confidence: 99%
“…It is given by the value at which m PCAC = 0. Instead of determining it ourselves, we use very precise critical masses obtained in [26,27]. These were computed from slightly different correlation functions in a finite volume, and differ from ours by an O(a) lattice artifact.…”
Section: Pcac Massmentioning
confidence: 99%
“…The spatial dimensions are kept periodic. Moreover, for the production of our ensembles we benefit from the knowledge of the critical mass m cr [30,31] and the axial current and pseudoscalar density renormalization factors Z A [32][33][34] and Z P [30,35]. For further details about the simulations we refer to our previous works [12,22] and references therein.…”
Section: Numerical Setupmentioning
confidence: 99%
“…To achieve maximal twist, the hopping parameter κ has been set to its critical value by interpolating the data published in Refs. [6,7]. Open boundary conditions in the temporal direction are imposed to keep auto-correlation times associated with the topological charge manageable [8].…”
Section: Numerical Setupmentioning
confidence: 99%