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  4. First observation and branching fraction measurement of the Λ b 0 → D s − p $$ {\Lambda}_b^0\to {D}_s^{-}p $$ decay

First observation and branching fraction measurement of the Λ b 0 → D s − p $$ {\Lambda}_b^0\to {D}_s^{-}p $$ decay

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Author(s)
Aaij, R.
•
Abdelmotteleb, A. S. W.
•
Abellan Beteta, C.
•
Abudinén, F.
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Ackernley, T.
•
Adeva, B.
•
Adinolfi, M.
•
Adlarson, P.
•
Afsharnia, H.
•
Agapopoulou, C.
more
Date Issued
July 10, 2023
Publisher
Springer Berlin Heidelberg
Citation
Journal of High Energy Physics. 2023 Jul 10;2023(7):75
Version
Final published version
Abstract
Abstract The first observation of the Λ b 0 → D s − p $$ {\Lambda}_b^0\to {D}_s^{-}p $$ decay is presented using proton-proton collision data collected by the LHCb experiment at a centre-of-mass energy of s $$ \sqrt{s} $$ = 13 TeV, corresponding to a total integrated luminosity of 6 fb−1. Using the Λ b 0 → Λ c + π − $$ {\Lambda}_b^0\to {\Lambda}_c^{+}{\pi}^{-} $$ decay as the normalisation mode, the branching fraction of the Λ b 0 → D s − p $$ {\Lambda}_b^0\to {D}_s^{-}p $$ decay is measured to be B Λ b 0 → D s − p = 12.6 ± 0.5 ± 0.3 ± 1.2 × 10 − 6 $$ \mathcal{B}\left({\Lambda}_b^0\to {D}_s^{-}p\right)=\left(12.6\pm 0.5\pm 0.3\pm 1.2\right)\times {10}^{-6} $$ , where the first uncertainty is statistical, the second systematic and the third due to uncertainties in the branching fractions of the Λ b 0 → Λ c + π − $$ {\Lambda}_b^0\to {\Lambda}_c^{+}{\pi}^{-} $$ , D s − → K − K + π − $$ {D}_s^{-}\to {K}^{-}{K}^{+}{\pi}^{-} $$ and Λ c + → p K − π + $$ {\Lambda}_c^{+}\to p{K}^{-}{\pi}^{+} $$ decays.
MIT Department
Massachusetts Institute of Technology. Department of Physics
Terms of Use
Creative Commons Attribution
http://creativecommons.org/licenses/by/4.0/
Persistent DSpace Link
https://hdl.handle.net/1721.1/151132
DOI of Published Version
https://doi.org/10.1007/JHEP07(2023)075
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