Study of light-meson resonances decaying to K S 0 K π in the B → ( K S 0 K π ) K channels

Aaij, R.; Abdelmotteleb, A. S. W.; Abellan Beteta, C.; Abudinén, F.; Ackernley, T.; Adefisoye, A. A.; Adeva, B.; Adinolfi, M.; Adlarson, P.; Agapopoulou, C.; Aidala, C. A.; Ajaltouni, Z.; Akar, S.; Akiba, K.; Albicocco, P.; Albrecht, J.; Alessio, F.; Alexander, M.; Aliouche, Z.; Alvarez Cartelle, P.; Amalric, R.; Amato, S.; Amey, J. L.; Amhis, Y.; An, L.; Anderlini, L.; Andersson, M.; Andreianov, A.; Andreola, P.; Andreotti, M.; Andreou, D.; Anelli, A.; Ao, D.; Archilli, F.; Argenton, M.; Arguedas Cuendis, S.; Artamonov, A.; Artuso, M.; Aslanides, E.; Ataíde Da Silva, R.; Atzeni, M.; Audurier, B.; Bacher, D.; Bachiller Perea, I.; Bachmann, S.; Bachmayer, M.; Back, J. J.; Baladron Rodriguez, P.; Balagura, V.; Balboni, A.; Baldini, W.; Balzani, L.; Bao, H.; Baptista de Souza Leite, J.; Barbero Pretel, C.; Barbetti, M.; Barbosa, I. R.; Barlow, R. J.; Barnyakov, M.; Barsuk, S.; Barter, W.; Bartz, J.; Basels, J. M.; Bashir, S.; Bassi, G.; Batsukh, B.; Battista, P. 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doi:10.1103/PhysRevD.111.092009

Study of light-meson resonances decaying to $K_{S}^{0} K π$ in the $B \to (K_{S}^{0} K π) K$ channels

Journal Article · Thu May 15 00:00:00 EDT 2025 · Physical Review. D.

DOI:https://doi.org/10.1103/PhysRevD.111.092009· OSTI ID:2566610

; ; Abellan Beteta, C.; ; ; ; ; ; ; ; ; Ajaltouni, Z.; ; ; ; ; ; ; ; more »

A study is presented of $B^{+} \to K_{S}^{0} K^{-} π^{+} K^{+}$ and $B^{+} \to K_{S}^{0} K^{+} π^{-} K^{+}$ decays based on the analysis of proton-proton collision data collected with the LHCb detector at center-of-mass energies of 7, 8 and 13 TeV, corresponding to an integrated luminosity of $9 {fb}^{- 1}$ . The $K_{S}^{0} K π$ invariant-mass distributions of both $B^{+}$ decay modes show, in the $m (K_{S}^{0} K π) < 1.85 GeV$ mass region, large activity which is resolved using an amplitude analysis. A simple model, where $J^{P C}$ amplitudes are described by multiple Breit-Wigner functions with appropriate angular distributions, provides a good description of the experimental data. In this approach a complex mixture of $J^{P C} = 0^{- +}$ , $1^{+ +}$ and $1^{+ -}$ amplitudes is observed that is dominated by $η (1405)$ , $η (1470)$ , $η (1760)$ , $f_{1} (1285)$ , $f_{1} (1420)$ and $h_{1} (1405)$ resonances. The $K_{S}^{0} K π$ Dalitz plots are dominated by asymmetric crossing $K^{*} \bar{K}$ bands which are different for the two $B^{+}$ decay modes. This is due to a different interference pattern between the $1^{+ +}$ and $1^{+ -}$ amplitudes in the two channels. Branching fractions are measured for each resonant contribution.

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Sponsoring Organization:: USDOE Office of Science (SC), Nuclear Physics (NP)

OSTI ID:: 2566610

Journal Information:: Physical Review. D., Journal Name: Physical Review. D. Journal Issue: 9 Vol. 111; ISSN PRVDAQ; ISSN 2470-0010

Publisher:: American Physical SocietyCopyright Statement

Country of Publication:: United States

Language:: English

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