Abstract
Abstract
We update the full set of $$ \overline{B} $$
B
¯
s → K form factors using light-cone sum rules with an on-shell kaon. Our approach determines the relevant sum rule parameters — the duality thresholds — from a Bayesian fit for the first time. Using a modified version of the Boyd-Grinstein-Lebed parametrisation, we combine our sum rule results at low momentum transfer q2 with more precise lattice QCD results at large q2. We obtain a consistent description of the form factors in the full q2 range. Applying these results to a recent LHCb measurement of branching ratios for the decays $$ {B}_s^0 $$
B
s
0
→ {K−, $$ {D}_s^{-} $$
D
s
−
}μ+νμ, we determine the ratio of Cabibbo-Kobayashi-Maskawa elements$$ {\left|\frac{V_{ub}}{V_{cb}}\right|}_{q^2<7\;{\textrm{GeV}}^2}=0.0681\pm 0.0040\kern0.5em \textrm{and}\kern0.5em {\left|\frac{V_{ub}}{V_{cb}}\right|}_{q^2>7\;{\textrm{GeV}}^2}=0.0801\pm 0.0047, $$
V
ub
V
cb
q
2
<
7
GeV
2
=
0.0681
±
0.0040
and
V
ub
V
cb
q
2
>
7
GeV
2
=
0.0801
±
0.0047
,
which are mutually compatible at the 1.9σ level. We further comment on the sensitivity to Beyond the Standard Model effects through measurements of the shape of $$ {B}_s^0 $$
B
s
0
→ K−μ+νμ decays, in light of recent limits on such effects from other exclusive b → uℓν processes.
Publisher
Springer Science and Business Media LLC
Subject
Nuclear and High Energy Physics
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