First measurement of the differential branching fraction and CP asymmetry of the B± → π±μ+μ− decay

被引:0
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作者
R. Aaij
B. Adeva
M. Adinolfi
A. Affolder
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
J. Anderson
G. Andreassi
M. Andreotti
J. E. Andrews
R. B. Appleby
O. Aquines Gutierrez
F. Archilli
P. d’Argent
A. Artamonov
M. Artuso
E. Aslanides
G. Auriemma
M. Baalouch
S. Bachmann
J. J. Back
A. Badalov
C. Baesso
W. Baldini
R. J. Barlow
C. Barschel
S. Barsuk
W. Barter
V. Batozskaya
V. Battista
A. Bay
L. Beaucourt
J. Beddow
F. Bedeschi
I. Bediaga
L. J. Bel
V. Bellee
N. Belloli
机构
[1] Centro Brasileiro de Pesquisas Físicas (CBPF),Center for High Energy Physics
[2] Universidade Federal do Rio de Janeiro (UFRJ),Fakultät Physik
[3] Tsinghua University,Physikalisches Institut
[4] LAPP,School of Physics
[5] Université Savoie Mont-Blanc,Physik
[6] CNRS/IN2P3,Institut
[7] Clermont Université,H.H. Wills Physics Laboratory
[8] Université Blaise Pascal,Cavendish Laboratory
[9] CNRS/IN2P3,Department of Physics
[10] LPC,School of Physics and Astronomy
[11] CPPM,School of Physics and Astronomy
[12] Aix-Marseille Université,Oliver Lodge Laboratory
[13] CNRS/IN2P3,School of Physics and Astronomy
[14] LAL,Department of Physics
[15] Université Paris-Sud,Institute of Particle Physics
[16] CNRS/IN2P3,Departamento de Fisica
[17] LPNHE,Institut für Physik
[18] Université Pierre et Marie Curie,Van Swinderen Institute
[19] Université Paris Diderot,P.N. Lebedev Physical Institute
[20] CNRS/IN2P3,LIFAELS, La Salle
[21] Technische Universität Dortmund,undefined
[22] Max-Planck-Institut für Kernphysik (MPIK),undefined
[23] Ruprecht-Karls-Universität Heidelberg,undefined
[24] University College Dublin,undefined
[25] Sezione INFN di Bari,undefined
[26] Sezione INFN di Bologna,undefined
[27] Sezione INFN di Cagliari,undefined
[28] Sezione INFN di Ferrara,undefined
[29] Sezione INFN di Firenze,undefined
[30] Laboratori Nazionali dell’INFN di Frascati,undefined
[31] Sezione INFN di Genova,undefined
[32] Sezione INFN di Milano Bicocca,undefined
[33] Sezione INFN di Milano,undefined
[34] Sezione INFN di Padova,undefined
[35] Sezione INFN di Pisa,undefined
[36] Sezione INFN di Roma Tor Vergata,undefined
[37] Sezione INFN di Roma La Sapienza,undefined
[38] Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences,undefined
[39] AGH - University of Science and Technology,undefined
[40] Faculty of Physics and Applied Computer Science,undefined
[41] National Center for Nuclear Research (NCBJ),undefined
[42] Horia Hulubei National Institute of Physics and Nuclear Engineering,undefined
[43] Petersburg Nuclear Physics Institute (PNPI),undefined
[44] Institute of Theoretical and Experimental Physics (ITEP),undefined
[45] Institute of Nuclear Physics,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
来源
Journal of High Energy Physics | / 2015卷
关键词
Rare decay; CP violation; Hadron-Hadron Scattering; Branching fraction; B physics;
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摘要
The differential branching fraction with respect to the dimuon invariant mass squared, and the CP asymmetry of the B± → π±μ+μ− decay are measured for the first time. The CKM matrix elements |Vtd| and |Vts|, and the ratio |Vtd/Vts| are determined. The analysis is performed using proton-proton collision data corresponding to an integrated luminosity of 3.0 fb−1, collected by the LHCb experiment at centre-of-mass energies of 7 and 8 TeV. The total branching fraction and CP asymmetry of B± → π±μ+μ− decays are measured to be ℬB±→π±μ+μ−=1.83±0.24±0.05×10−8andACPB±→π±μ+μ−=−0.11±0.12±0.01,\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \begin{array}{l}\mathrm{\mathcal{B}}\left({B}^{\pm}\to {\pi}^{\pm }{\mu}^{+}{\mu}^{-}\right)=\left(1.83\pm 0.24\pm 0.05\right)\times {10^{-}}^8\;\mathrm{and}\hfill \\ {}{\mathcal{A}}_{CP}\left({B}^{\pm}\to {\pi}^{\pm }{\mu}^{+}{\mu}^{-}\right)=-0.11\pm 0.12\pm 0.01,\hfill \end{array} $$\end{document} where the first uncertainties are statistical and the second are systematic. These are the most precise measurements of these observables to date, and they are compatible with the predictions of the Standard Model. [graphic not available: see fulltext]
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