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  4. Observation of the semileptonic decay B+→pp¯μ+νμ$$ {B}^{+}\to p\overline{p}{\mu}^{+}{\nu}_{\mu } $$

Observation of the semileptonic decay B+→pp¯μ+νμ$$ {B}^{+}\to p\overline{p}{\mu}^{+}{\nu}_{\mu } $$

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Author(s)
Aaij, R.
•
Abellán Beteta, C.
•
Ackernley, T.
•
Adeva, B.
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Adinolfi, M.
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Afsharnia, H.
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Aidala, C. A
•
Aiola, S.
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Ajaltouni, Z.
•
Akar, S.
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Date Issued
March 25, 2020
Publisher
Springer Berlin Heidelberg
Citation
Journal of High Energy Physics. 2020 Mar 25;2020(3):146
Version
Final published version
Abstract
Abstract The Cabibbo-suppressed semileptonic decay B+→pp¯μ+νμ$$ {B}^{+}\to p\overline{p}{\mu}^{+}{\nu}_{\mu } $$ is observed for the first time using a sample of pp collisions corresponding to an integrated luminosity of 1.0, 2.0 and 1.7 fb−1 at centre-of-mass energies of 7, 8 and 13 TeV, respectively. The differential branching fraction is measured as a function of the pp¯$$ p\overline{p} $$ invariant mass using the decay mode B+→ J/ψK+ for normalisation. The total branching fraction is measured to be ℬ B + → p p ¯ μ + ν μ = 5.27 − 0.24 + 0.23 ± 0.21 ± 0.15 × 10 − 6 , $$ \mathrm{\mathcal{B}}\left({B}^{+}\to p\overline{p}{\mu}^{+}{\nu}_{\mu}\right)=\left({5.27}_{-0.24}^{+0.23}\pm 0.21\pm 0.15\right)\times {10}^{-6}, $$ where the first uncertainty is statistical, the second systematic and the third is from the uncertainty on the branching fraction of the normalisation channel.
MIT Department
Massachusetts Institute of Technology. Department of Physics
Terms of Use
Creative Commons Attribution
https://creativecommons.org/licenses/by/4.0/
Persistent DSpace Link
https://hdl.handle.net/1721.1/131694
DOI of Published Version
https://doi.org/10.1007/JHEP03(2020)146
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