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3 Tests of lepton universality
Lepton universality tests probe the Standard Model prediction that the
charged weak current interaction has the same coupling for all lepton generations.
The precision of such tests has been significantly improved since the
2014 edition by the
addition of the Belle τ lifetime
measurement [67], while improvements from the τ branching fraction fit are negligible.
We compute the universality tests as in the previous report by using
ratios of the partial widths of a heavier lepton λ
decaying to a lighter lepton ρ [68],
| Γ(λ → νλ ρ | | ρ (γ)) =
| | =
| | f | ⎛
⎜
⎜
⎝ | | ⎞
⎟
⎟
⎠ |
RWλ Rγλ ,
|
| | | | | | | | | | |
|
where
| Gρ | | | |
f(x) | = 1 −8x +8x3 −x4 −12x2 lnx , | |
RWλ | | | |
Rγλ | | |
|
We use Rγτ=1−43.2· 10−4 and
Rγµ=1−42.4· 10−4 [68] and MW
from PDG 2015 [8].
We use HFAG 2014 averages and PDG 2015 for the other quantities.
Using pure leptonic processes we obtain
| | ⎛
⎜
⎜
⎝ | | | ⎞
⎟
⎟
⎠ | = 1.0010 ± 0.0015 , |
| | | ⎛
⎜
⎜
⎝ | | | ⎞
⎟
⎟
⎠ | = 1.0029 ± 0.0015 , |
| | | ⎛
⎜
⎜
⎝ | | | ⎞
⎟
⎟
⎠ | = 1.0019 ± 0.0014 .
|
| | | | | | |
|
Using the expressions for the τ semi-hadronic partial widths [69] we obtain
| | ⎛
⎜
⎜
⎝ | | | ⎞
⎟
⎟
⎠ | | =
| |
| 2mh mµ2τh |
|
(1 + δ Rτ/h)mτ3ττ |
|
| ⎛
⎜
⎜
⎝ | | | ⎞
⎟
⎟
⎠ | | ,
|
| | | | | | | | | | |
|
where h = π or K and the radiative corrections are
δ Rτ/π = (0.16 ± 0.12)% and
δ Rτ/K = (0.90 ± 0.22)% [69],
we measure:
| | = 0.9961 ± 0.0027 , | | ⎛
⎜
⎜
⎝ | | | ⎞
⎟
⎟
⎠ | | = 0.9860 ± 0.0070 .
|
| | | | | | | | |
|
Similar tests could be performed with decays to electrons, however they are
less precise because the hadron two body decays to electrons are
helicity-suppressed.
Averaging the three gτ/gµ ratios we obtain
accounting for statistical correlations.
Table 12 reports the statistical correlation coefficients for the fitted coupling ratios:
Table 12: Universality coupling ratios correlation coefficients (%). |
|
( gτ/ge ) | 53 |
( gµ/ge ) | -49 | 48 |
( gτ/gµ )π | 24 | 26 | 2 |
( gτ/gµ )K | 11 | 10 | -1 | 6 |
| ( gτ/gµ ) | ( gτ/ge ) | ( gµ/ge ) | ( gτ/gµ )π
|
|
Since there is 100% correlation between gτ/ge,
gµ/ge and gµ/ge, the correlation matrix is expected to be
positive semi-definite, with one eigenvalue equal to zero. Due to
numerical inaccuracies, one eigenvalue is expected to be close to zero
rather than exactly zero.
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