Measurement of CP observables in B± → D(*)K± and B± → D(*)π± decays using two-body D final states

被引:0
作者
R. Aaij
C. Abellán Beteta
T. Ackernley
B. Adeva
M. Adinolfi
H. Afsharnia
C. A. Aidala
S. Aiola
Z. Ajaltouni
S. Akar
J. Albrecht
F. Alessio
M. Alexander
A. Alfonso Albero
Z. Aliouche
G. Alkhazov
P. Alvarez Cartelle
S. Amato
Y. Amhis
L. An
L. Anderlini
A. Andreianov
M. Andreotti
F. Archilli
A. Artamonov
M. Artuso
K. Arzymatov
E. Aslanides
M. Atzeni
B. Audurier
S. Bachmann
M. Bachmayer
J. J. Back
S. Baker
P. Baladron Rodriguez
V. Balagura
W. Baldini
J. Baptista Leite
R. J. Barlow
S. Barsuk
W. Barter
M. Bartolini
F. Baryshnikov
J. M. Basels
G. Bassi
B. Batsukh
A. Battig
A. Bay
M. Becker
F. Bedeschi
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 State Key Laboratory of Nuclear Physics and Technology
[3] Tsinghua University,Institute of Particle Physics
[4] Peking University,I. Physikalisches Institut
[5] University of Chinese Academy of Sciences,Fakultät Physik
[6] Institute Of High Energy Physics (IHEP),Physikalisches Institut
[7] Central China Normal University,School of Physics
[8] Université Grenoble Alpes,ICCUB
[9] Université Savoie Mont Blanc,Instituto Galego de Física de Altas Enerxías (IGFAE)
[10] CNRS,Physik
[11] IN2P3-LAPP,Institut
[12] Université Clermont Auvergne,H.H. Wills Physics Laboratory
[13] CNRS/IN2P3,Cavendish Laboratory
[14] LPC,Department of Physics
[15] Aix Marseille Univ,School of Physics and Astronomy
[16] CNRS/IN2P3,School of Physics and Astronomy
[17] CPPM,Oliver Lodge Laboratory
[18] Université Paris-Saclay,Department of Physics and Astronomy
[19] CNRS/IN2P3,Department of Physics
[20] IJCLab,School of Physics and Astronomy
[21] Laboratoire Leprince-ringuet (llr),Physics and Micro Electronic College
[22] LPNHE,Guangdong Provencial Key Laboratory of Nuclear Science, Institute of Quantum Matter
[23] Sorbonne Université,School of Physics and Technology
[24] Paris Diderot Sorbonne Paris Cité,Departamento de Fisica
[25] CNRS/IN2P3,Institut für Physik
[26] RWTH Aachen University,Van Swinderen Institute
[27] Technische Universität Dortmund,DS4DS, La Salle
[28] Max-Planck-Institut für Kernphysik (MPIK),undefined
[29] Ruprecht-Karls-Universität Heidelberg,undefined
[30] University College Dublin,undefined
[31] INFN Sezione di Bari,undefined
[32] INFN Sezione di Bologna,undefined
[33] INFN Sezione di Ferrara,undefined
[34] INFN Sezione di Firenze,undefined
[35] INFN Laboratori Nazionali di Frascati,undefined
[36] INFN Sezione di Genova,undefined
[37] INFN Sezione di Milano-Bicocca,undefined
[38] INFN Sezione di Milano,undefined
[39] INFN Sezione di Cagliari,undefined
[40] Universita degli Studi di Padova,undefined
[41] Universita e INFN,undefined
[42] Padova,undefined
[43] INFN Sezione di Pisa,undefined
[44] INFN Sezione di Roma Tor Vergata,undefined
[45] INFN Sezione di Roma La Sapienza,undefined
[46] Nikhef National Institute for Subatomic Physics,undefined
[47] Nikhef National Institute for Subatomic Physics and VU University Amsterdam,undefined
[48] Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences,undefined
[49] AGH — University of Science and Technology,undefined
[50] Faculty of Physics and Applied Computer Science,undefined
来源
Journal of High Energy Physics | / 2021卷
关键词
physics; CKM angle gamma; CP violation; Hadron-Hadron scattering (experiments);
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摘要
Measurements of CP observables in B± → D(*)K± and B± → D(*)π± decays are presented, where D(∗) indicates a neutral D or D∗ meson that is an admixture of meson and anti-meson states. Decays of the D(∗) meson to the Dπ0 and Dγ final states are partially reconstructed without inclusion of the neutral pion or photon. Decays of the D meson are reconstructed in the K±π∓, K+K−, and π+π− final states. The analysis uses a sample of charged B mesons produced in proton-proton collisions and collected with the LHCb experiment, corresponding to integrated luminosities of 2.0, 1.0, and 5.7 fb−1 taken at centre-of-mass energies of 7, 8, and 13 TeV, respectively. The measurements of partially reconstructed B± → D(*)K± and B± → D(∗)π± with D → K∓π± decays are the first of their kind, and a first observation of the B± → Dπ0D∗π±\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {\left(D{\pi}^0\right)}_{D^{\ast }}{\pi}^{\pm } $$\end{document} decay is made with a significance of 6.1 standard deviations. All CP observables are measured with world-best precision, and in combination with other LHCb results will provide strong constraints on the CKM angle γ.
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