Observation of the decay Bs0 → ηcϕ and evidence for Bs0 → ηcπ+π−

被引:0
作者
R. Aaij
B. Adeva
M. Adinolfi
Z. Ajaltouni
S. Akar
J. Albrecht
F. Alessio
M. Alexander
S. Ali
G. Alkhazov
P. Alvarez Cartelle
A. A. Alves
S. Amato
S. Amerio
Y. Amhis
L. An
L. Anderlini
G. Andreassi
M. Andreotti
J. E. Andrews
R. B. Appleby
F. Archilli
P. d’Argent
J. Arnau Romeu
A. Artamonov
M. Artuso
E. Aslanides
G. Auriemma
M. Baalouch
I. Babuschkin
S. Bachmann
J. J. Back
A. Badalov
C. Baesso
S. Baker
V. Balagura
W. Baldini
R. J. Barlow
C. Barschel
S. Barsuk
W. Barter
F. Baryshnikov
M. Baszczyk
V. Batozskaya
B. Batsukh
V. Battista
A. Bay
L. Beaucourt
J. Beddow
F. Bedeschi
机构
[1] Centro Brasileiro de Pesquisas Físicas (CBPF),Center for High Energy Physics
[2] Universidade Federal do Rio de Janeiro (UFRJ),I. Physikalisches Institut
[3] Tsinghua University,Fakultät Physik
[4] LAPP,Physikalisches Institut
[5] Université Savoie Mont-Blanc,School of Physics
[6] CNRS/IN2P3,Physik
[7] Clermont Université,Institut
[8] Université Blaise Pascal,H.H. Wills Physics Laboratory
[9] CNRS/IN2P3,Cavendish Laboratory
[10] LPC,Department of Physics
[11] CPPM,School of Physics and Astronomy
[12] Aix-Marseille Université,School of Physics and Astronomy
[13] CNRS/IN2P3,Oliver Lodge Laboratory
[14] LAL,School of Physics and Astronomy
[15] Université Paris-Sud,Department of Physics
[16] CNRS/IN2P3,School of Physics and Technology
[17] LPNHE,Institute of Particle Physics
[18] Université Pierre et Marie Curie,Departamento de Fisica
[19] Université Paris Diderot,Institut für Physik
[20] CNRS/IN2P3,Van Swinderen Institute
[21] RWTH Aachen University,LIFAELS, La Salle
[22] Technische Universität Dortmund,undefined
[23] Max-Planck-Institut für Kernphysik (MPIK),undefined
[24] Ruprecht-Karls-Universität Heidelberg,undefined
[25] University College Dublin,undefined
[26] Sezione INFN di Bari,undefined
[27] Sezione INFN di Bologna,undefined
[28] Sezione INFN di Cagliari,undefined
[29] Sezione INFN di Ferrara,undefined
[30] Sezione INFN di Firenze,undefined
[31] Laboratori Nazionali dell’INFN di Frascati,undefined
[32] Sezione INFN di Genova,undefined
[33] Sezione INFN di Milano Bicocca,undefined
[34] Sezione INFN di Milano,undefined
[35] Sezione INFN di Padova,undefined
[36] Sezione INFN di Pisa,undefined
[37] Sezione INFN di Roma Tor Vergata,undefined
[38] Sezione INFN di Roma La Sapienza,undefined
[39] Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences,undefined
[40] AGH - University of Science and Technology,undefined
[41] Faculty of Physics and Applied Computer Science,undefined
[42] National Center for Nuclear Research (NCBJ),undefined
[43] Horia Hulubei National Institute of Physics and Nuclear Engineering,undefined
[44] Petersburg Nuclear Physics Institute (PNPI),undefined
[45] Institute of Theoretical and Experimental Physics (ITEP),undefined
[46] Institute of Nuclear Physics,undefined
[47] Moscow State University (SINP MSU),undefined
[48] Institute for Nuclear Research of the Russian Academy of Sciences (INR RAN),undefined
[49] Yandex School of Data Analysis,undefined
[50] Budker Institute of Nuclear Physics (SB RAS),undefined
来源
Journal of High Energy Physics | / 2017卷
关键词
B physics; Branching fraction; Flavor physics; Hadron-Hadron scattering (experiments);
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摘要
A study of Bs0 → ηcϕ and Bs0 → ηcπ+π− decays is performed using pp collision data corresponding to an integrated luminosity of 3.0 fb−1, collected with the LHCb detector in Run 1 of the LHC. The observation of the decay Bs0 → ηcϕ is reported, where the ηc meson is reconstructed in the pp¯\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ p\overline{p} $$\end{document}, K+K−π+π−, π+π−π+π− and K+K−K+K− decay modes and the ϕ(1020) in the K+K− decay mode. The decay Bs0 → J/ψϕ is used as a normalisation channel. Evidence is also reported for the decay Bs0 → ηcπ+π−, where the ηc meson is reconstructed in the pp¯\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ p\overline{p} $$\end{document} decay mode, using the decay Bs0 → J/ψπ+π− as a normalisation channel. The measured branching fractions are ℬBs0→ηcϕ=5.01±0.53±0.27±0.63×10−4,ℬBs0→ηcπ+π−=1.76±0.59±0.12±0.29×10−4,\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \begin{array}{l}\mathrm{\mathcal{B}}\left({B}_s^0\to {\eta}_c\phi \right)=\left(5.01\pm 0.53\pm 0.27\pm 0.63\right)\times {10}^{-4},\hfill \\ {}\mathrm{\mathcal{B}}\left({B}_s^0\to {\eta}_c{\pi}^{+}{\pi}^{-}\right)=\left(1.76\pm 0.59\pm 0.12\pm 0.29\right)\times {10}^{-4},\hfill \end{array} $$\end{document} where in each case the first uncertainty is statistical, the second systematic and the third uncertainty is due to the limited knowledge of the external branching fractions. [graphic not available: see fulltext]
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