Observation of the decays B0 (s) → Ds1(2536)∓K±

This paper reports the observation of the decays B0 (s) → Ds1(2536)∓K± using proton-proton collision data collected by the LHCb experiment, corresponding to an integrated luminosity of 9 fb−1 . The branching fractions of these decays are measured relative to the normalisation channel B0 → D 0K+K−. T...

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Detalles Bibliográficos
Autores: Valls Canudas, Núria, Calvo Gomez, Miriam, Vilasis-Cardona, Xavier, Golobardes Ribé, Elisabet, LHCb Collaboration - CERN
Tipo de recurso: artículo
Fecha de publicación:2023
País:España
Institución:Universitat Ramon Llull (URL)
Repositorio:DAU Arxiu Digital de la Universitat Ramon Llull
OAI Identifier:oai:dnet:dau_________::524d016f2a78bab3b5bbc9d659c16cc7
Acceso en línea:https://hdl.handle.net/20.500.14342/6449
https://doi.org/10.1007/JHEP10(2023)106
Access Level:acceso abierto
Palabra clave:B Physics
Branching fraction
Flavour Physics
Hadron-Hadron Scattering
Decay Processes
Experimental Nuclear Physics
Nuclear Physics
Gran col·lisionador d'hadrons
51
53
539
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oai_identifier_str oai:dnet:dau_________::524d016f2a78bab3b5bbc9d659c16cc7
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spelling Observation of the decays B0 (s) → Ds1(2536)∓K±Valls Canudas, NúriaCalvo Gomez, MiriamVilasis-Cardona, XavierGolobardes Ribé, ElisabetLHCb Collaboration - CERNB PhysicsBranching fractionFlavour PhysicsHadron-Hadron ScatteringDecay ProcessesExperimental Nuclear PhysicsNuclear PhysicsGran col·lisionador d'hadrons5153539This paper reports the observation of the decays B0 (s) → Ds1(2536)∓K± using proton-proton collision data collected by the LHCb experiment, corresponding to an integrated luminosity of 9 fb−1 . The branching fractions of these decays are measured relative to the normalisation channel B0 → D 0K+K−. The Ds1(2536)− meson is reconstructed in the D ∗ (2007)0K− decay channel and the products of branching fractions are measured to be B(B 0 s → Ds1(2536)∓K±) × B(Ds1(2536)−→ D ∗ (2007)0K−) = (2.49 ± 0.11 ± 0.12 ± 0.25 ± 0.06) × 10−5 , B(B 0→ Ds1(2536)∓K±) × B(Ds1(2536)−→ D ∗ (2007)0K−) = (0.510 ± 0.021 ± 0.036 ± 0.050) × 10−5 . The first uncertainty is statistical, the second systematic, and the third arises from the uncertainty of the branching fraction of the B0 → D 0K+K− normalisation channel. The last uncertainty in the B0 s result is due to the limited knowledge of the fragmentation fraction ratio, fs/fd. The significance for the B0 s and B0 signals is larger than 10 σ. The ratio of the helicity amplitudes which governs the angular distribution of the Ds1(2536)− → D ∗ (2007)0K− decay is determined from the data. The ratio of the S- and D-wave amplitudes is found to be 1.11±0.15±0.06 and the phase difference between them 0.70 ± 0.09 ± 0.04 rad, where the first uncertainty is statistical and the second systematic.info:eu-repo/semantics/publishedVersionSpringer NatureUniversitat Ramon Llull. La SalleCERN2026202620232023info:eu-repo/semantics/article25 p.application/pdfhttps://hdl.handle.net/20.500.14342/6449https://doi.org/10.1007/JHEP10(2023)106reponame:DAU Arxiu Digital de la Universitat Ramon Llullinstname:Universitat Ramon Llull (URL)InglésJournal of High Energy Physics, 2023, Vol. 2023, 106© CERNAttribution 4.0 Internationalhttp://creativecommons.org/licenses/by/4.0/info:eu-repo/semantics/openAccessoai:dnet:dau_________::524d016f2a78bab3b5bbc9d659c16cc72026-06-21T06:40:37Z
dc.title.none.fl_str_mv Observation of the decays B0 (s) → Ds1(2536)∓K±
title Observation of the decays B0 (s) → Ds1(2536)∓K±
spellingShingle Observation of the decays B0 (s) → Ds1(2536)∓K±
Valls Canudas, Núria
B Physics
Branching fraction
Flavour Physics
Hadron-Hadron Scattering
Decay Processes
Experimental Nuclear Physics
Nuclear Physics
Gran col·lisionador d'hadrons
51
53
539
title_short Observation of the decays B0 (s) → Ds1(2536)∓K±
title_full Observation of the decays B0 (s) → Ds1(2536)∓K±
title_fullStr Observation of the decays B0 (s) → Ds1(2536)∓K±
title_full_unstemmed Observation of the decays B0 (s) → Ds1(2536)∓K±
title_sort Observation of the decays B0 (s) → Ds1(2536)∓K±
dc.creator.none.fl_str_mv Valls Canudas, Núria
Calvo Gomez, Miriam
Vilasis-Cardona, Xavier
Golobardes Ribé, Elisabet
LHCb Collaboration - CERN
author Valls Canudas, Núria
author_facet Valls Canudas, Núria
Calvo Gomez, Miriam
Vilasis-Cardona, Xavier
Golobardes Ribé, Elisabet
LHCb Collaboration - CERN
author_role author
author2 Calvo Gomez, Miriam
Vilasis-Cardona, Xavier
Golobardes Ribé, Elisabet
LHCb Collaboration - CERN
author2_role author
author
author
author
dc.contributor.none.fl_str_mv Universitat Ramon Llull. La Salle
CERN
dc.subject.none.fl_str_mv B Physics
Branching fraction
Flavour Physics
Hadron-Hadron Scattering
Decay Processes
Experimental Nuclear Physics
Nuclear Physics
Gran col·lisionador d'hadrons
51
53
539
topic B Physics
Branching fraction
Flavour Physics
Hadron-Hadron Scattering
Decay Processes
Experimental Nuclear Physics
Nuclear Physics
Gran col·lisionador d'hadrons
51
53
539
description This paper reports the observation of the decays B0 (s) → Ds1(2536)∓K± using proton-proton collision data collected by the LHCb experiment, corresponding to an integrated luminosity of 9 fb−1 . The branching fractions of these decays are measured relative to the normalisation channel B0 → D 0K+K−. The Ds1(2536)− meson is reconstructed in the D ∗ (2007)0K− decay channel and the products of branching fractions are measured to be B(B 0 s → Ds1(2536)∓K±) × B(Ds1(2536)−→ D ∗ (2007)0K−) = (2.49 ± 0.11 ± 0.12 ± 0.25 ± 0.06) × 10−5 , B(B 0→ Ds1(2536)∓K±) × B(Ds1(2536)−→ D ∗ (2007)0K−) = (0.510 ± 0.021 ± 0.036 ± 0.050) × 10−5 . The first uncertainty is statistical, the second systematic, and the third arises from the uncertainty of the branching fraction of the B0 → D 0K+K− normalisation channel. The last uncertainty in the B0 s result is due to the limited knowledge of the fragmentation fraction ratio, fs/fd. The significance for the B0 s and B0 signals is larger than 10 σ. The ratio of the helicity amplitudes which governs the angular distribution of the Ds1(2536)− → D ∗ (2007)0K− decay is determined from the data. The ratio of the S- and D-wave amplitudes is found to be 1.11±0.15±0.06 and the phase difference between them 0.70 ± 0.09 ± 0.04 rad, where the first uncertainty is statistical and the second systematic.
publishDate 2023
dc.date.none.fl_str_mv 2023
2023
2026
2026
dc.type.none.fl_str_mv info:eu-repo/semantics/article
format article
dc.identifier.none.fl_str_mv https://hdl.handle.net/20.500.14342/6449
https://doi.org/10.1007/JHEP10(2023)106
url https://hdl.handle.net/20.500.14342/6449
https://doi.org/10.1007/JHEP10(2023)106
dc.language.none.fl_str_mv Inglés
language_invalid_str_mv Inglés
dc.relation.none.fl_str_mv Journal of High Energy Physics, 2023, Vol. 2023, 106
dc.rights.none.fl_str_mv © CERN
Attribution 4.0 International
http://creativecommons.org/licenses/by/4.0/
info:eu-repo/semantics/openAccess
rights_invalid_str_mv © CERN
Attribution 4.0 International
http://creativecommons.org/licenses/by/4.0/
eu_rights_str_mv openAccess
dc.format.none.fl_str_mv 25 p.
application/pdf
dc.publisher.none.fl_str_mv Springer Nature
publisher.none.fl_str_mv Springer Nature
dc.source.none.fl_str_mv reponame:DAU Arxiu Digital de la Universitat Ramon Llull
instname:Universitat Ramon Llull (URL)
instname_str Universitat Ramon Llull (URL)
reponame_str DAU Arxiu Digital de la Universitat Ramon Llull
collection DAU Arxiu Digital de la Universitat Ramon Llull
repository.name.fl_str_mv
repository.mail.fl_str_mv
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