The first observation of the decay Ξžβˆ’π‘β†’πœ“β‘(2⁒𝑆)β’Ξžβˆ’ and measurement of the branching ratio of Ξžβˆ’ π‘β†’πœ“β‘(2⁒𝑆)β’Ξžβˆ’ to Ξžβˆ’π‘β†’π½/πœ“β’Ξžβˆ’ are presented. The 𝐽/πœ“ and πœ“β‘(2⁒𝑆) mesons are reconstructed using their dimuon decay modes. The results are based on proton-proton colliding beam data from the LHC collected by the CMS experiment at βˆšπ‘ =13  TeV in 2016–2018, corresponding to an integrated luminosity of 140  fbβˆ’1. The branching fraction ratio is measured to be ℬ⁑(Ξžβˆ’ π‘β†’πœ“β‘(2⁒𝑆)β’Ξžβˆ’)/ℬ⁑(Ξžβˆ’π‘β†’π½/πœ“β’Ξžβˆ’)=0.8⁒4+0.21βˆ’0.19⁒(stat)Β±0.10⁒(syst)Β±0.02⁒(ℬ), where the last uncertainty comes from the uncertainties in the branching fractions of the charmonium states. New measurements of the Ξžπ‘β’(5945)0 baryon mass and natural width are also presented, using the Ξžβˆ’ π‘β’πœ‹+ final state, where the Ξžβˆ’π‘ baryon is reconstructed through the decays 𝐽/πœ“β’Ξžβˆ’, πœ“β‘(2⁒𝑆)β’Ξžβˆ’, 𝐽/πœ“β’Ξ›β’πΎβˆ’, and 𝐽/πœ“β’Ξ£0β’πΎβˆ’. Finally, the fraction of Ξžβˆ’π‘ baryons produced from Ξžπ‘β’(5945)0 decays is determined.

Observation of the Xi_b- -> psi(2S) Xi- decay and studies of the Xi_b(5945)0 baryon in proton-proton collisions at sqrt(s) = 13 TeV / Belforte, S.; Candelise, V.; Casarsa, M.; Cossutti, F.; De Leo, K.; Della Ricca, G.; ET AL (the CMS, Collaboration); Vazzoler, F; Sorrentino, G. - In: PHYSICAL REVIEW D. - ISSN 2470-0010. - STAMPA. - 110:(2024), pp. 012002.1-012002.27. [10.1103/PhysRevD.110.012002]

Observation of the Xi_b- -> psi(2S) Xi- decay and studies of the Xi_b(5945)0 baryon in proton-proton collisions at sqrt(s) = 13 TeV

CANDELISE, V.;DE LEO, K.;DELLA RICCA, G.;VAZZOLER, F
Membro del Collaboration Group
;
SORRENTINO, G
Membro del Collaboration Group
2024-01-01

Abstract

The first observation of the decay Ξžβˆ’π‘β†’πœ“β‘(2⁒𝑆)β’Ξžβˆ’ and measurement of the branching ratio of Ξžβˆ’ π‘β†’πœ“β‘(2⁒𝑆)β’Ξžβˆ’ to Ξžβˆ’π‘β†’π½/πœ“β’Ξžβˆ’ are presented. The 𝐽/πœ“ and πœ“β‘(2⁒𝑆) mesons are reconstructed using their dimuon decay modes. The results are based on proton-proton colliding beam data from the LHC collected by the CMS experiment at βˆšπ‘ =13  TeV in 2016–2018, corresponding to an integrated luminosity of 140  fbβˆ’1. The branching fraction ratio is measured to be ℬ⁑(Ξžβˆ’ π‘β†’πœ“β‘(2⁒𝑆)β’Ξžβˆ’)/ℬ⁑(Ξžβˆ’π‘β†’π½/πœ“β’Ξžβˆ’)=0.8⁒4+0.21βˆ’0.19⁒(stat)Β±0.10⁒(syst)Β±0.02⁒(ℬ), where the last uncertainty comes from the uncertainties in the branching fractions of the charmonium states. New measurements of the Ξžπ‘β’(5945)0 baryon mass and natural width are also presented, using the Ξžβˆ’ π‘β’πœ‹+ final state, where the Ξžβˆ’π‘ baryon is reconstructed through the decays 𝐽/πœ“β’Ξžβˆ’, πœ“β‘(2⁒𝑆)β’Ξžβˆ’, 𝐽/πœ“β’Ξ›β’πΎβˆ’, and 𝐽/πœ“β’Ξ£0β’πΎβˆ’. Finally, the fraction of Ξžβˆ’π‘ baryons produced from Ξžπ‘β’(5945)0 decays is determined.
2024
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11368/3080618
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