Searches for \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$ B_{(s)}^0\ \to {J \left/ {{\psi p}} \right.}\overline{p} $\end{document} and B+→ J/ψ p\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$ \overline{p} $\end{document}π+ decays

被引:0
作者
R. Aaij
B. Adeva
M. Adinolfi
C. Adrover
A. Affolder
Z. Ajaltouni
J. Albrecht
F. Alessio
M. Alexander
S. Ali
G. Alkhazov
P. Alvarez Cartelle
A. A. Alves
S. Amato
S. Amerio
Y. Amhis
L. Anderlini
J. Anderson
R. Andreassen
J. E. Andrews
R. B. Appleby
O. Aquines Gutierrez
F. Archilli
A. Artamonov
M. Artuso
E. Aslanides
G. Auriemma
M. Baalouch
S. Bachmann
J. J. Back
C. Baesso
V. Balagura
W. Baldini
R. J. Barlow
C. Barschel
S. Barsuk
W. Barter
Th. Bauer
A. Bay
J. Beddow
F. Bedeschi
I. Bediaga
S. Belogurov
K. Belous
I. Belyaev
E. Ben-Haim
G. Bencivenni
S. Benson
J. Benton
A. Berezhnoy
机构
[1] Centro Brasileiro de Pesquisas Físicas (CBPF),Center for High Energy Physics
[2] Universidade Federal do Rio de Janeiro (UFRJ),School of Physics
[3] Tsinghua University,Institute of Nuclear Physics
[4] LAPP,Physik
[5] Université de Savoie,Institut
[6] CNRS/IN2P3,H.H. Wills Physics Laboratory
[7] Clermont Université,Cavendish Laboratory
[8] Université Blaise Pascal,Department of Physics
[9] CNRS/IN2P3,School of Physics and Astronomy
[10] LPC,School of Physics and Astronomy
[11] CPPM,Oliver Lodge Laboratory
[12] Aix-Marseille Université,School of Physics and Astronomy
[13] CNRS/IN2P3,Department of Physics
[14] LAL,undefined
[15] Université Paris-Sud,undefined
[16] CNRS/IN2P3,undefined
[17] LPNHE,undefined
[18] Université Pierre et Marie Curie,undefined
[19] Université Paris Diderot,undefined
[20] CNRS/IN2P3,undefined
[21] Fakultät Physik,undefined
[22] Technische Universität Dortmund,undefined
[23] Max-Planck-Institut für Kernphysik (MPIK),undefined
[24] Physikalisches Institut,undefined
[25] Ruprecht-Karls-Universität Heidelberg,undefined
[26] University College Dublin,undefined
[27] Sezione INFN di Bari,undefined
[28] Sezione INFN di Bologna,undefined
[29] Sezione INFN di Cagliari,undefined
[30] Sezione INFN di Ferrara,undefined
[31] Sezione INFN di Firenze,undefined
[32] Laboratori Nazionali dell’INFN di Frascati,undefined
[33] Sezione INFN di Genova,undefined
[34] Sezione INFN di Milano Bicocca,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] Moscow State University (SINP MSU),undefined
[47] Institute for Nuclear Research of the Russian Academy of Sciences (INR RAN),undefined
[48] Budker Institute of Nuclear Physics (SB RAS) and Novosibirsk State University,undefined
[49] Institute for High Energy Physics (IHEP),undefined
[50] Universitat de Barcelona,undefined
关键词
Hadron-Hadron Scattering; Branching fraction; B physics; Flavor physics;
D O I
10.1007/JHEP09(2013)006
中图分类号
学科分类号
摘要
The results of searches for \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$ B_{(s)}^0\to {J \left/ {\psi\ p } \right.}\overline{p} $\end{document} and B+ → J/ψ p\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$ \overline{p} $\end{document}π+ decays are reported. The analysis is based on a data sample, corresponding to an integrated luminosity of 1.0 fb−1 of pp collisions, collected with the LHCb detector. An excess with 2.8 σ significance is seen for the decay \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$ B_s^0\to {J \left/ {\psi\ p } \right.}\overline{p} $\end{document} and an upper limit on the branching fraction is set at the 90 % confidence level: \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$ \mathcal{B}\left( {B_s^0\to {J \left/ {\psi\ p } \right.}\overline{p}} \right) $\end{document}< 4.8 × 10−6, which is the first such limit. No significant signals are seen for B0 → J/ψ p\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$ \overline{p} $\end{document} and B+ → J/ψ p\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$ \overline{p} $\end{document}π+ decays, for which the corresponding limits are set: \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$ \mathcal{B}\left( {{B^0}\to {J \left/ {\psi\ p } \right.}\overline{p}} \right) $\end{document}< 5.2 × 10−7, which significantly improves the existing limit; and \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$ \mathcal{B}\left( {{B^{+}}\to {J \left/ {\psi\ p } \right.}\overline{p}{\pi^{+}}} \right) $\end{document}< 5.0 × 10−7, which is the first limit on this branching fraction.
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