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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.accessioned2023-07-17T14:04:31Z
dc.date.available2023-07-17T14:04:31Z
dc.date.issued2023-07-07
dc.identifier.urihttps://hdl.handle.net/1721.1/151130
dc.description.abstractAbstract The ratio of branching fractions of B c + → B s 0 π + $$ {B}_c^{+}\to {B}_s^0{\pi}^{+} $$ and B c + → J / ψ π + $$ {B}_c^{+}\to J/\psi {\pi}^{+} $$ decays is measured with proton-proton collision data of a centre-of-mass energy of 13 TeV. The data were collected with the LHCb experiment during 2016–2018, corresponding to an integrated luminosity of 5.4 fb−1. The B s 0 $$ {B}_s^0 $$ mesons are reconstructed via the decays B s 0 → J / ψϕ $$ {B}_s^0\to J/\psi \phi $$ and B s 0 → D s − π + $$ {B}_s^0\to {D}_s^{-}{\pi}^{+} $$ . The ratio of branching fractions is measured to be B B c + → B s 0 π + / B B c + → J / ψ π + = 91 ± 10 ± 8 ± 3 $$ \mathcal{B}\left({B}_c^{+}\to {B}_s^0{\pi}^{+}\right)/\mathcal{B}\left({B}_c^{+}\to J/\psi {\pi}^{+}\right)=91\pm 10\pm 8\pm 3 $$ where the first uncertainty is statistical, the second is systematic and the third is due to the knowledge of the branching fractions of the intermediate state decays.en_US
dc.publisherSpringer Berlin Heidelbergen_US
dc.relation.isversionofhttps://doi.org/10.1007/JHEP07(2023)066en_US
dc.rightsCreative Commons Attributionen_US
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/en_US
dc.sourceSpringer Berlin Heidelbergen_US
dc.titleMeasurement of the ratio of branching fractions B B c + → B s 0 π + / B B c + → J / ψ π + $$ \mathcal{B}\left({B}_c^{+}\to {B}_s^0{\pi}^{+}\right)/\mathcal{B}\left({B}_c^{+}\to J/\psi {\pi}^{+}\right) $$en_US
dc.typeArticleen_US
dc.identifier.citationJournal of High Energy Physics. 2023 Jul 07;2023(7):66en_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.updated2023-07-16T03:10:57Z
dc.language.rfc3066en
dc.rights.holderThe Author(s)
dspace.embargo.termsN
dspace.date.submission2023-07-16T03:10:57Z
mit.licensePUBLISHER_CC
mit.metadata.statusAuthority Work and Publication Information Neededen_US


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