Model-independent measurement of the CKM angle γ using B0 → DK∗0 decays with D → KS0π+π− and KS0K+K−

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作者
R. Aaij
C. Abellán Beteta
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
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
S. Baker
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),LPNHE, Université Pierre et Marie Curie
[3] Tsinghua University,I. Physikalisches Institut
[4] LAPP,Fakultät Physik
[5] Université Savoie Mont-Blanc,Physikalisches Institut
[6] CNRS/IN2P3,School of Physics
[7] Clermont Université,Institute of Nuclear Physics
[8] Université Blaise Pascal,Physik
[9] CNRS/IN2P3,Institut
[10] LPC,H.H. Wills Physics Laboratory
[11] CPPM,Cavendish Laboratory
[12] Aix-Marseille Université,Department of Physics
[13] CNRS/IN2P3,School of Physics and Astronomy
[14] LAL,School of Physics and Astronomy
[15] Université Paris-Sud,Oliver Lodge Laboratory
[16] CNRS/IN2P3,School of Physics and Astronomy
[17] Université Paris Diderot,Department of Physics
[18] CNRS/IN2P3,Institute of Particle Physics
[19] RWTH Aachen University,Departamento de Fisica
[20] Technische Universität Dortmund,Institut für Physik
[21] Max-Planck-Institut für Kernphysik (MPIK),Instituto de Fisica Corpuscular (IFIC)
[22] Ruprecht-Karls-Universität Heidelberg,Van Swinderen Institute
[23] University College Dublin,P.N. Lebedev Physical Institute
[24] Sezione INFN di Bari,undefined
[25] Sezione INFN di Bologna,undefined
[26] Sezione INFN di Cagliari,undefined
[27] Sezione INFN di Ferrara,undefined
[28] Sezione INFN di Firenze,undefined
[29] Laboratori Nazionali dell’INFN di Frascati,undefined
[30] Sezione INFN di Genova,undefined
[31] Sezione INFN di Milano Bicocca,undefined
[32] Sezione INFN di Milano,undefined
[33] Sezione INFN di Padova,undefined
[34] Sezione INFN di Pisa,undefined
[35] Sezione INFN di Roma Tor Vergata,undefined
[36] Sezione INFN di Roma La Sapienza,undefined
[37] Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences,undefined
[38] AGH - University of Science and Technology,undefined
[39] Faculty of Physics and Applied Computer Science,undefined
[40] National Center for Nuclear Research (NCBJ),undefined
[41] Horia Hulubei National Institute of Physics and Nuclear Engineering,undefined
[42] Petersburg Nuclear Physics Institute (PNPI),undefined
[43] Institute of Theoretical and Experimental Physics (ITEP),undefined
[44] Moscow State University (SINP MSU),undefined
[45] Institute for Nuclear Research of the Russian Academy of Sciences (INR RAN),undefined
[46] Budker Institute of Nuclear Physics (SB RAS) and Novosibirsk State University,undefined
[47] Institute for High Energy Physics (IHEP),undefined
[48] Universitat de Barcelona,undefined
[49] Universidad de Santiago de Compostela,undefined
[50] European Organization for Nuclear Research (CERN),undefined
关键词
B physics; CKM angle gamma; CP violation; Flavor physics; Hadron-Hadron scattering (experiments);
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摘要
A binned Dalitz plot analysis of the decays B0 → DK∗0, with D → KS0π+π− and D → KS0K+K−, is performed to measure the observables x± and y±, which are related to the CKM angle γ and the hadronic parameters of the decays. The D decay strong phase variation over the Dalitz plot is taken from measurements performed at the CLEO-c experiment, making the analysis independent of the D decay model. With a sample of proton-proton collision data, corresponding to an integrated luminosity of 3.0 fb−1, collected by the LHCb experiment, the values of the CP violation parameters are found to be x+ = 0.05 ± 0.35 ± 0.02, x− = −0.31 ± 0.20 ± 0.04, y+ = −0.81 ± 0.28 ± 0.06 and y− = 0.31 ± 0.21 ± 0.05, where the first uncertainties are statistical and the second systematic. These observables correspond to values γ = (71 ± 20)°, rB0=0.56±0.17\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {r_B}_{{}^0}=0.56\pm 0.17 $$\end{document} and δB0=204−20+21°\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {\delta_B}_{{}^0}=\left(20{4}_{-20}^{+21}\right){}^{\circ} $$\end{document}. The parameters rB0\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {r_B}_{{}^0} $$\end{document} and δB0\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {\delta_B}_{{}^0} $$\end{document} are the magnitude ratio and strong phase difference between the suppressed and favoured B0 decay amplitudes, and have been measured in a region of ±50 MeV/c2 around the K∗(892)0 mass and with the magnitude of the cosine of the K∗(892)0 helicity angle larger than 0.4. [graphic not available: see fulltext]
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