Composite leptoquarks and anomalies in B-meson decays
A bstract We attempt to explain recent anomalies in semileptonic B decays at LHCb via a composite Higgs model, in which both the Higgs and an SU(2) L -triplet leptoquark arise as pseudo-Goldstone bosons of the strong dynamics. Fermion masses are assumed to be generated via the mechanism of partial c...
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Published in: | The journal of high energy physics Vol. 2015; no. 5; p. 1 |
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Main Authors: | , , |
Format: | Journal Article |
Language: | English |
Published: |
Berlin/Heidelberg
Springer Berlin Heidelberg
04-05-2015
Springer Nature B.V |
Subjects: | |
Online Access: | Get full text |
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Summary: | A
bstract
We attempt to explain recent anomalies in semileptonic
B
decays at LHCb via a composite Higgs model, in which both the Higgs and an SU(2)
L
-triplet leptoquark arise as pseudo-Goldstone bosons of the strong dynamics. Fermion masses are assumed to be generated via the mechanism of partial compositeness, which largely determines the leptoquark couplings and implies non-universal lepton interactions. The latter are needed to accommodate tensions in the
b
→
sμμ
dataset and to be consistent with a discrepancy measured at LHCb in the ratio of
B
+
→
K
+
μ
+
μ
−
to
B
+
→
K
+
e
+
e
−
branching ratios. The data imply that the leptoquark should have a mass of around a TeV. We find that the model is not in conflict with current flavour or direct production bounds, but we identify a few observables for which the new physics contributions are close to current limits and where the leptoquark is likely to show up in future measurements. The leptoquark will be pair-produced at the LHC and decay predominantly to third-generation quarks and leptons, and LHC13 searches will provide further strong bounds. |
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ISSN: | 1029-8479 1029-8479 |
DOI: | 10.1007/JHEP05(2015)006 |