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dc.contributor.authorAaij, R.
dc.contributor.authorAbdelmotteleb, A. S. W.
dc.contributor.authorAbellan Beteta, C.
dc.contributor.authorAbudinén, F.
dc.contributor.authorAckernley, T.
dc.contributor.authorAdeva, B.
dc.contributor.authorAdinolfi, M.
dc.contributor.authorAdlarson, P.
dc.contributor.authorAfsharnia, H.
dc.contributor.authorAgapopoulou, C.
dc.contributor.authorAidala, C. A.
dc.contributor.authorAjaltouni, Z.
dc.contributor.authorAkar, S.
dc.contributor.authorAkiba, K.
dc.contributor.authorAlbicocco, P.
dc.contributor.authorAlbrecht, J.
dc.date.accessioned2023-07-17T14:08:20Z
dc.date.available2023-07-17T14:08:20Z
dc.date.issued2023-07-10
dc.identifier.urihttps://hdl.handle.net/1721.1/151132
dc.description.abstractAbstract 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.en_US
dc.publisherSpringer Berlin Heidelbergen_US
dc.relation.isversionofhttps://doi.org/10.1007/JHEP07(2023)075en_US
dc.rightsCreative Commons Attributionen_US
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/en_US
dc.sourceSpringer Berlin Heidelbergen_US
dc.titleFirst observation and branching fraction measurement of the Λ b 0 → D s − p $$ {\Lambda}_b^0\to {D}_s^{-}p $$ decayen_US
dc.typeArticleen_US
dc.identifier.citationJournal of High Energy Physics. 2023 Jul 10;2023(7):75en_US
dc.contributor.departmentMassachusetts Institute of Technology. Department of Physics
dc.identifier.mitlicensePUBLISHER_CC
dc.eprint.versionFinal published versionen_US
dc.type.urihttp://purl.org/eprint/type/JournalArticleen_US
eprint.statushttp://purl.org/eprint/status/PeerRevieweden_US
dc.date.updated2023-07-16T03:11:04Z
dc.language.rfc3066en
dc.rights.holderThe Author(s)
dspace.embargo.termsN
dspace.date.submission2023-07-16T03:11:04Z
mit.licensePUBLISHER_CC
mit.metadata.statusAuthority Work and Publication Information Neededen_US


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