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Probing new physics in class-I B-meson decays into heavy-light final states
A bstract With updated experimental data and improved theoretical calculations, several significant deviations are being observed between the Standard Model predictions and the experimental measurements of the branching ratios of B ¯ s 0 → D s ∗ + L − decays, where L is a light meson from the set {...
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Published in: | The journal of high energy physics 2021-10, Vol.2021 (10), p.1-49, Article 235 |
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Main Authors: | , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | A
bstract
With updated experimental data and improved theoretical calculations, several significant deviations are being observed between the Standard Model predictions and the experimental measurements of the branching ratios of
B
¯
s
0
→
D
s
∗
+
L
−
decays, where
L
is a light meson from the set {
π
,
ρ
,
K
(∗)
}. Especially for the two channels
B
¯
0
→
D
+
K
−
and
B
¯
s
0
→
D
s
+
π
−
, both of which are free of the weak annihilation contribution, the deviations observed can even reach 4–5
σ
. Here we exploit possible new-physics effects in these class-I non-leptonic
B
-meson decays within the framework of QCD factorization. Firstly, we perform a model-independent analysis of the effects from twenty linearly independent four-quark operators that can contribute, either directly or through operator mixing, to the quark-level
b →
c
u
¯
d
s
transitions. It is found that, under the combined constraints from the current experimental data, the deviations observed could be well explained at the 1
σ
level by the new-physics four-quark operators with
γ
μ
(1
− γ
5
) ⨂
γ
μ
(1
− γ
5
) structure, and also at the 2
σ
level by the operators with (1 +
γ
5
) ⨂ (1
− γ
5
) and (1 +
γ
5
) ⨂ (1 +
γ
5
) structures. However, the new-physics four-quark operators with other Dirac structures fail to provide a consistent interpretation, even at the 2
σ
level. Then, as two specific examples of model-dependent considerations, we discuss the case where the new-physics four-quark operators are generated by either a colorless charged gauge boson or a colorless charged scalar, with their masses fixed both at the 1 TeV. Constraints on the effective coefficients describing the couplings of these mediators to the relevant quarks are obtained by fitting to the current experimental data. |
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ISSN: | 1029-8479 1029-8479 |
DOI: | 10.1007/JHEP10(2021)235 |