The branching fraction of leptonic decays of pseudo-scalar mesons
that proceed via the annihilation of the initial quark-antiquark pair (cd
in the case of D+ meson) into a virtual W+ that finally materializes as an antilepton-neutrino pair (lν, where l = e, μ, or τ) is
given in the Standard Model by
Mode | Branching Fraction | fD|Vcd| (MeV) | Experiment | Source |
---|---|---|---|---|
μ+ ν | (3.82 ± 0.32 ± 0.09) × 10-4 | 46.4 ± 1.9 ± 0.5 ± 0.2 | CLEO | B. I. Eisenstein et al. (CLEO Collaboration), Phys. Rev. D 78, 052003 (2008) |
(3.71 ± 0.19 ± 0.06) × 10-4 | 45.7 ± 1.2 ± 0.4 ± 0.2 | BESIII | M. Ablikim et al. (BESIII Collaboration), Phys. Rev. D 89, 051104 (2014) | |
(3.74 ± 0.16 ± 0.05) × 10-4 | 45.9 ± 1.0 ± 0.3 ± 0.2 | HFAG Average | ||
e+ ν | < 8.8 × 10-6 at 90% C.L. | CLEO | B. I. Eisenstein et al. (CLEO Collaboration), Phys. Rev. D 78, 052003 (2008) | |
τ+ ν | < 1.2 × 10-3 at 90% C.L. |
We use measurements of the branching fraction Br(D+→ μ+ν) from CLEO
and BESIII to calculate its world average (WA) value. Uncertainties of the two measurements are considered to be uncorrelated. We obtain
Assuming unitarity of the CKM matrix, the value of the element relevant in the case of leptonic D+ decays
is known from the global fit of the CKM matrix, |Vcd| = 0.22537+0.00068-0.00035. This value can be used to extract
the D meson decay constant from the experimentally measured product fD|Vcd|.
This leads to the experimentally measured D meson decay constant to be:
External parameter values as taken from the 2014 Particle Data Book:
and the
second error is the systematic error. (Click on figure for higher resolution.)
GF /(ℏc)3 =
(1.1663787 ± 0.0000006) × 10-5 GeV-2
Mμ = (0.1056583715 ± 0.0000000035) GeV/c2
MD = (1.86962 ± 0.00015) GeV/c2
τD = (1040 ± 7) × 10-15 s
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