TY - JOUR
T1 - Lattice QCD calculation of B̄→Dlv̄ decay form factors at zero recoil
AU - Hashimoto, Shoji
AU - El-Khadra, Aida X.
AU - Kronfeld, Andreas S.
AU - Mackenzie, Paul B.
AU - Ryan, Sinéad M.
AU - Simone, James N.
PY - 2000/1/1
Y1 - 2000/1/1
N2 - A lattice QCD calculation of the B̄→Dlv̄ decay form factors is presented. We obtain the value of the form factor h+(w) at the zero-recoil limit w=1 with high precision by considering a ratio of correlation functions in which the bulk of the uncertainties cancels. The other form factor h_(w) is calculated, for small recoil momenta, from a similar ratio. In both cases, the heavy quark mass dependence is observed through direct calculations with several combinations of initial and final heavy quark masses. Our results are h+(1) = 1.007(6)(2)(3) and h_(1)=-0.107(28)(04)(3010). For both the first error is statistical; the second stems from the uncertainty in adjusting the heavy quark masses and the last from omitted radiative corrections. Combining these results, we obtain a precise determination of the physical combination ℱB→D(1) = 1.058(1720), where the mentioned systematic errors are added in quadrature. The dependence on lattice spacing and the effect of quenching are not yet included, but with our method they should be a fraction of ℱB→D-1.
AB - A lattice QCD calculation of the B̄→Dlv̄ decay form factors is presented. We obtain the value of the form factor h+(w) at the zero-recoil limit w=1 with high precision by considering a ratio of correlation functions in which the bulk of the uncertainties cancels. The other form factor h_(w) is calculated, for small recoil momenta, from a similar ratio. In both cases, the heavy quark mass dependence is observed through direct calculations with several combinations of initial and final heavy quark masses. Our results are h+(1) = 1.007(6)(2)(3) and h_(1)=-0.107(28)(04)(3010). For both the first error is statistical; the second stems from the uncertainty in adjusting the heavy quark masses and the last from omitted radiative corrections. Combining these results, we obtain a precise determination of the physical combination ℱB→D(1) = 1.058(1720), where the mentioned systematic errors are added in quadrature. The dependence on lattice spacing and the effect of quenching are not yet included, but with our method they should be a fraction of ℱB→D-1.
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U2 - 10.1103/PhysRevD.61.014502
DO - 10.1103/PhysRevD.61.014502
M3 - Article
AN - SCOPUS:16644373542
SN - 0556-2821
VL - 61
SP - 1
EP - 13
JO - Physical Review D - Particles, Fields, Gravitation and Cosmology
JF - Physical Review D - Particles, Fields, Gravitation and Cosmology
IS - 1
M1 - 014502
ER -